id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
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values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0712.3224 | Anastasios Avgoustidis | A. Avgoustidis | Cosmic String Dynamics and Evolution in Warped Spacetime | 21 pages, 5 figures; Discussion section expanded, physical
implications further explored; To appear in PRD | Phys.Rev.D78:023501,2008 | 10.1103/PhysRevD.78.023501 | UB-ECM-PF-07/35, DAMTP-2007-121 | hep-th astro-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the dynamics and evolution of Nambu-Goto strings in a warped
spacetime, where the warp factor is a function of the internal coordinates
giving rise to a `throat' region. The microscopic equations of motion for
strings in this background include potential and friction terms, which attract
the strings towards ... | [
{
"created": "Wed, 19 Dec 2007 16:15:10 GMT",
"version": "v1"
},
{
"created": "Wed, 11 Jun 2008 15:05:10 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Avgoustidis",
"A.",
""
]
] | We study the dynamics and evolution of Nambu-Goto strings in a warped spacetime, where the warp factor is a function of the internal coordinates giving rise to a `throat' region. The microscopic equations of motion for strings in this background include potential and friction terms, which attract the strings towards th... | 13.764262 | 13.483789 | 14.567923 | 12.833907 | 14.560124 | 12.379443 | 12.999225 | 12.676059 | 13.027091 | 13.719983 | 12.764484 | 13.330108 | 12.687034 | 12.843179 | 12.924479 | 13.161119 | 13.075656 | 12.489928 | 12.544293 | 12.530298 | 13.075126 |
hep-th/0211217 | Cheol Ryou | Youngjai Kiem, Yoonbai Kim, Jaemo Park, Cheol Ryou | Chiral primary cubic interactions from pp-wave supergravity | 14 pages, A few comments are added | JHEP 0301 (2003) 026 | 10.1088/1126-6708/2003/01/026 | null | hep-th | null | We explicitly construct cubic interaction light-cone Hamiltonian for the
chiral primary system involving the metric fields and the self-dual four-form
fields in the IIB pp-wave supergravity. The background fields representing
pp-waves exhibit SO(4)*SO(4)*Z_2 invariance. It turns out that the interaction
Hamiltonian i... | [
{
"created": "Fri, 22 Nov 2002 14:37:58 GMT",
"version": "v1"
},
{
"created": "Tue, 28 Jan 2003 10:49:39 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Kiem",
"Youngjai",
""
],
[
"Kim",
"Yoonbai",
""
],
[
"Park",
"Jaemo",
""
],
[
"Ryou",
"Cheol",
""
]
] | We explicitly construct cubic interaction light-cone Hamiltonian for the chiral primary system involving the metric fields and the self-dual four-form fields in the IIB pp-wave supergravity. The background fields representing pp-waves exhibit SO(4)*SO(4)*Z_2 invariance. It turns out that the interaction Hamiltonian is ... | 10.222122 | 9.39715 | 10.337717 | 8.743019 | 9.341274 | 9.326164 | 9.627989 | 8.632096 | 9.236711 | 11.728574 | 8.774157 | 8.537482 | 9.756294 | 9.254992 | 8.126053 | 8.969419 | 8.631367 | 8.958727 | 9.007464 | 9.618527 | 8.569727 |
1105.0481 | Prasanta K. Tripathy | Pramod Dominic and Prasanta K. Tripathy | On the Stability of Non-Supersymmetric Quantum Attractors in String
Theory | References Added, Typos Corrected, Appendix A.2 Reordered | null | 10.1007/JHEP06(2011)112 | IITM/PH/TH/2011/4 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study four dimensional non-supersymmetric attractors in type IIA string
theory in the presence of sub-leading corrections to the prepotential. For a
given Calabi-Yau manifold, the D0-D4 system admits an attractor point in the
moduli space which is uniquely specified by the black hole charges. The
perturbative corr... | [
{
"created": "Tue, 3 May 2011 06:10:34 GMT",
"version": "v1"
},
{
"created": "Wed, 4 May 2011 19:48:00 GMT",
"version": "v2"
},
{
"created": "Sat, 7 May 2011 14:39:06 GMT",
"version": "v3"
}
] | 2015-05-28 | [
[
"Dominic",
"Pramod",
""
],
[
"Tripathy",
"Prasanta K.",
""
]
] | We study four dimensional non-supersymmetric attractors in type IIA string theory in the presence of sub-leading corrections to the prepotential. For a given Calabi-Yau manifold, the D0-D4 system admits an attractor point in the moduli space which is uniquely specified by the black hole charges. The perturbative correc... | 6.120644 | 5.304115 | 6.69759 | 5.460881 | 6.026244 | 5.611522 | 5.735969 | 5.252941 | 5.610191 | 6.867408 | 5.415753 | 5.585466 | 6.067833 | 5.894336 | 5.939857 | 5.899194 | 5.781247 | 5.64861 | 6.002387 | 5.967426 | 5.757578 |
2403.10594 | Shruti Paranjape | Christoph Bartsch, Taro V. Brown, Karol Kampf, Umut Oktem, Shruti
Paranjape, Jaroslav Trnka | Hidden Amplitude Zeros From Double Copy | 1 figure, 2 tables | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Recently, Arkani-Hamed et al. proposed the existence of zeros in scattering
amplitudes in certain quantum field theories including the cubic adjoint scalar
theory Tr($\phi^3$), the $SU(N)$ non-linear sigma model (NLSM) and Yang-Mills
(YM) theory. These hidden zeros are special kinematic points where the
amplitude van... | [
{
"created": "Fri, 15 Mar 2024 18:00:00 GMT",
"version": "v1"
}
] | 2024-03-19 | [
[
"Bartsch",
"Christoph",
""
],
[
"Brown",
"Taro V.",
""
],
[
"Kampf",
"Karol",
""
],
[
"Oktem",
"Umut",
""
],
[
"Paranjape",
"Shruti",
""
],
[
"Trnka",
"Jaroslav",
""
]
] | Recently, Arkani-Hamed et al. proposed the existence of zeros in scattering amplitudes in certain quantum field theories including the cubic adjoint scalar theory Tr($\phi^3$), the $SU(N)$ non-linear sigma model (NLSM) and Yang-Mills (YM) theory. These hidden zeros are special kinematic points where the amplitude vanis... | 7.273136 | 6.24083 | 7.66021 | 6.307148 | 6.674705 | 6.622334 | 6.319045 | 6.185618 | 6.01086 | 8.640171 | 6.647913 | 6.602395 | 6.97519 | 6.567267 | 6.783865 | 6.651752 | 6.58177 | 6.545608 | 6.686132 | 7.03055 | 6.697658 |
0910.4898 | Paul Heslop | Andreas Brandhuber, Paul Heslop, Valentin V. Khoze, Gabriele
Travaglini | Simplicity of Polygon Wilson Loops in N=4 SYM | 28 pages, 11 figures, pdflatex. v2 minor typos corrected | JHEP 1001:050,2010 | 10.1007/JHEP01(2010)050 | IPPP/09/83, DCPT/09/166, QMUL-PH-09-23 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Wilson loops with lightlike polygonal contours have been conjectured to be
equivalent to MHV scattering amplitudes in N=4 super Yang-Mills. We compute
such Wilson loops for special polygonal contours at two loops in perturbation
theory. Specifically, we concentrate on the remainder function R, obtained by
subtracting... | [
{
"created": "Mon, 26 Oct 2009 14:54:06 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Jun 2010 12:21:42 GMT",
"version": "v2"
}
] | 2010-06-29 | [
[
"Brandhuber",
"Andreas",
""
],
[
"Heslop",
"Paul",
""
],
[
"Khoze",
"Valentin V.",
""
],
[
"Travaglini",
"Gabriele",
""
]
] | Wilson loops with lightlike polygonal contours have been conjectured to be equivalent to MHV scattering amplitudes in N=4 super Yang-Mills. We compute such Wilson loops for special polygonal contours at two loops in perturbation theory. Specifically, we concentrate on the remainder function R, obtained by subtracting t... | 7.698762 | 6.953243 | 8.678497 | 7.013568 | 7.378803 | 7.613032 | 7.155097 | 6.777768 | 6.916232 | 9.135925 | 7.321272 | 7.264776 | 7.559191 | 7.272016 | 7.481199 | 7.298144 | 7.495554 | 7.098376 | 7.328434 | 7.742499 | 7.089439 |
hep-th/0210089 | Matthias Blau | Giovanni Arcioni, Matthias Blau, Martin O'Loughlin | On the Boundary Dynamics of Chern-Simons Gravity | 22 pages, LaTeX2e, v2: JHEP3.cls, references and a footnote added | JHEP 0301:067,2003 | 10.1088/1126-6708/2003/01/067 | null | hep-th gr-qc | null | We study Chern-Simons theory with a complex G_C or a real G x G gauge group
on a manifold with boundary - this includes Lorentzian and Euclidean (anti-) de
Sitter (E/A)dS gravity for G=SU(2) or G=SL(2,R). We show that there is a
canonical choice of boundary conditions that leads to an unambiguous, fully
covariant and... | [
{
"created": "Wed, 9 Oct 2002 19:05:41 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Dec 2002 17:27:43 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Arcioni",
"Giovanni",
""
],
[
"Blau",
"Matthias",
""
],
[
"O'Loughlin",
"Martin",
""
]
] | We study Chern-Simons theory with a complex G_C or a real G x G gauge group on a manifold with boundary - this includes Lorentzian and Euclidean (anti-) de Sitter (E/A)dS gravity for G=SU(2) or G=SL(2,R). We show that there is a canonical choice of boundary conditions that leads to an unambiguous, fully covariant and g... | 9.863558 | 11.169813 | 10.562934 | 10.049283 | 9.915364 | 10.42543 | 10.678129 | 10.626267 | 9.917166 | 12.398674 | 10.001739 | 9.955035 | 10.181317 | 9.740366 | 9.734815 | 10.001057 | 9.683615 | 9.895436 | 9.755198 | 10.866594 | 9.571318 |
0909.2219 | Sante Carloni Dr | Sante Carloni, Emilio Elizalde, Pedro J. Silva | An analysis of the phase space of Horava-Lifshitz cosmologies | 12 pages, some typos corrected, some references added | null | 10.1088/0264-9381/27/4/045004 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using the dynamical system approach, properties of cosmological models based
on the Horava-Lifshitz gravity are systematically studied. In particular, the
cosmological phase space of the Horava-Lifshitz model is characterized. The
analysis allows to compare some key physical consequences of the imposition (or
not) of... | [
{
"created": "Fri, 11 Sep 2009 19:04:36 GMT",
"version": "v1"
},
{
"created": "Mon, 26 Oct 2009 14:22:45 GMT",
"version": "v2"
}
] | 2015-05-14 | [
[
"Carloni",
"Sante",
""
],
[
"Elizalde",
"Emilio",
""
],
[
"Silva",
"Pedro J.",
""
]
] | Using the dynamical system approach, properties of cosmological models based on the Horava-Lifshitz gravity are systematically studied. In particular, the cosmological phase space of the Horava-Lifshitz model is characterized. The analysis allows to compare some key physical consequences of the imposition (or not) of d... | 9.235453 | 9.945354 | 9.073698 | 8.795933 | 9.300279 | 9.557435 | 9.331522 | 9.118118 | 8.993684 | 9.483394 | 9.19201 | 9.046893 | 9.125593 | 8.799392 | 8.920656 | 8.729363 | 8.919182 | 8.878038 | 9.33281 | 9.087271 | 8.805307 |
hep-th/0608067 | Peter Orland | Peter Orland | String Tensions and Representations in Anisotropic 2+1-Dimensional
Weakly-Coupled Yang-Mills Theory | Some added clarifications included. Now ten pages | Phys.Rev.D75:025001,2007 | 10.1103/PhysRevD.75.025001 | BCCUNY-HEP/06-03 | hep-th cond-mat.str-el hep-lat | null | In earlier papers we established quark confinement analytically in
anisotropic $(2+1)$-dimensional Yang-Mills theory with two gauge coupling
constants. Here we point out a few features of the confining phase. These are:
1) the string tension in the $x^{2}$-direction as a function of representation
obeys a sine law, a... | [
{
"created": "Thu, 10 Aug 2006 09:57:57 GMT",
"version": "v1"
},
{
"created": "Sat, 19 Aug 2006 18:20:07 GMT",
"version": "v2"
},
{
"created": "Fri, 6 Oct 2006 18:58:36 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Orland",
"Peter",
""
]
] | In earlier papers we established quark confinement analytically in anisotropic $(2+1)$-dimensional Yang-Mills theory with two gauge coupling constants. Here we point out a few features of the confining phase. These are: 1) the string tension in the $x^{2}$-direction as a function of representation obeys a sine law, and... | 10.68037 | 10.438856 | 10.828904 | 11.010333 | 10.896567 | 9.888621 | 10.626346 | 9.730172 | 10.159104 | 10.638988 | 9.371443 | 9.722631 | 10.48313 | 10.28737 | 10.044933 | 9.712817 | 9.986913 | 9.948565 | 10.03761 | 10.186884 | 9.332457 |
hep-th/0202199 | Robertus Potting | Yu.A. Kubyshin, R. Neves and R. Potting | Solutions of the Polchinski ERG equation in the O(N) scalar model | 34 pages, 10 figures. References added. Version accepted for
publication in the International Journal of Modern Physics A | Int.J.Mod.Phys. A17 (2002) 4871-4902 | 10.1142/S0217751X02011400 | null | hep-th | null | Solutions of the Polchinski exact renormalization group equation in the
scalar O(N) theory are studied. Families of regular solutions are found and
their relation with fixed points of the theory is established. Special
attention is devoted to the limit $N=\infty$, where many properties can be
analyzed analytically.
| [
{
"created": "Wed, 27 Feb 2002 23:43:05 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Sep 2002 15:29:40 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Kubyshin",
"Yu. A.",
""
],
[
"Neves",
"R.",
""
],
[
"Potting",
"R.",
""
]
] | Solutions of the Polchinski exact renormalization group equation in the scalar O(N) theory are studied. Families of regular solutions are found and their relation with fixed points of the theory is established. Special attention is devoted to the limit $N=\infty$, where many properties can be analyzed analytically. | 8.642332 | 6.833098 | 7.69785 | 6.542166 | 7.02796 | 7.027023 | 6.814867 | 6.634995 | 6.612582 | 8.293789 | 6.509502 | 7.215629 | 7.248459 | 6.991829 | 7.071621 | 6.737326 | 6.679924 | 6.994174 | 7.103399 | 7.355439 | 6.863624 |
hep-th/0007094 | Emilio Elizalde | E. Elizalde | Matching the observational value of the cosmological constant | 13 pages, no figures, LaTeX | Phys.Lett. B516 (2001) 143-150 | 10.1016/S0370-2693(01)00921-2 | IEEC/CSM-00-63 | hep-th astro-ph gr-qc hep-ph | null | A simple model is introduced in which the cosmological constant is
interpreted as a true Casimir effect on a scalar field filling the universe
(e.g. $\mathbf{R} \times \mathbf{T}^p\times \mathbf{T}^q$, $\mathbf{R} \times
\mathbf{T}^p\times \mathbf{S}^q, ...$). The effect is driven by compactifying
boundary conditions... | [
{
"created": "Wed, 12 Jul 2000 15:19:04 GMT",
"version": "v1"
},
{
"created": "Tue, 15 May 2001 17:56:56 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Elizalde",
"E.",
""
]
] | A simple model is introduced in which the cosmological constant is interpreted as a true Casimir effect on a scalar field filling the universe (e.g. $\mathbf{R} \times \mathbf{T}^p\times \mathbf{T}^q$, $\mathbf{R} \times \mathbf{T}^p\times \mathbf{S}^q, ...$). The effect is driven by compactifying boundary conditions i... | 9.658388 | 9.814791 | 9.743409 | 9.346024 | 10.201765 | 9.99118 | 10.332007 | 9.451117 | 9.509932 | 9.686687 | 9.425506 | 9.256379 | 9.27243 | 9.239281 | 9.180793 | 9.229827 | 9.342463 | 9.252845 | 9.092699 | 9.243537 | 8.93891 |
1312.0895 | Andrey Sadofyev | V.P. Kirilin, A.V. Sadofyev, V.I. Zakharov | Anomaly and long-range forces | 14 pages, conference talk | null | 10.1142/9789814616850_0014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider infrared dependences of chiral effects, like chiral magnetic
effect, in chiral media. The main observation is that there exist competing
infrared-sensitive parameters, sometimes not apparent. The value of the chiral
effects depends in fact on the actual hierarchy of the parameters. Some
examples have been... | [
{
"created": "Tue, 3 Dec 2013 18:19:43 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Kirilin",
"V. P.",
""
],
[
"Sadofyev",
"A. V.",
""
],
[
"Zakharov",
"V. I.",
""
]
] | We consider infrared dependences of chiral effects, like chiral magnetic effect, in chiral media. The main observation is that there exist competing infrared-sensitive parameters, sometimes not apparent. The value of the chiral effects depends in fact on the actual hierarchy of the parameters. Some examples have been a... | 11.984135 | 10.480782 | 11.225504 | 11.098665 | 10.674294 | 10.150542 | 10.569749 | 10.871751 | 11.009284 | 12.763312 | 10.473344 | 10.637889 | 11.052141 | 10.475077 | 10.714015 | 10.987596 | 10.745187 | 10.932615 | 10.751452 | 11.414403 | 10.793102 |
2308.14704 | Atanu Bhatta | Atanu Bhatta, Shankhadeep Chakrabortty, Taniya Mandal, Arpit Maurya | Holographic Thermal Correlators for Hyperbolic $CFT$s | 17 pages, 7 tables, references added, matches the version published
in JHEP | null | 10.1007/JHEP11(2023)156 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use holography to compute the exact form of retarded Green's functions for
a scalar operator with conformal dimension $\Delta$ in a thermal CFT and in its
related counterpart with chemical potential in $R^1 \times H^3$. In our
analysis, we recast the wave equation of a scalar field in the normal form of
Heun's equ... | [
{
"created": "Mon, 28 Aug 2023 16:57:29 GMT",
"version": "v1"
},
{
"created": "Sun, 26 Nov 2023 14:24:26 GMT",
"version": "v2"
}
] | 2023-11-28 | [
[
"Bhatta",
"Atanu",
""
],
[
"Chakrabortty",
"Shankhadeep",
""
],
[
"Mandal",
"Taniya",
""
],
[
"Maurya",
"Arpit",
""
]
] | We use holography to compute the exact form of retarded Green's functions for a scalar operator with conformal dimension $\Delta$ in a thermal CFT and in its related counterpart with chemical potential in $R^1 \times H^3$. In our analysis, we recast the wave equation of a scalar field in the normal form of Heun's equat... | 10.143033 | 9.704069 | 10.799061 | 9.25404 | 9.483539 | 9.505333 | 9.791162 | 9.166943 | 9.376038 | 11.581774 | 9.476222 | 9.624896 | 10.541287 | 9.547743 | 9.561367 | 9.549133 | 9.64858 | 9.502183 | 9.646253 | 10.416642 | 9.475106 |
2310.07823 | Horatiu Stefan Nastase | Andr\'es Anabal\'on and Horatiu Nastase | Universal IR Holography, Scalar Fluctuations and Glueball spectra | 17 pages, 3 figures; reference added; clarifications added, published
version | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that the d'Alembertian operator with a possible mass term in the AdS
soliton and more general confining gravity dual backrounds admits infinitely
many different spectra. These can be interpreted as different theories in the
infrared and correspond to multitrace deformations of either the Dirichlet or
the Neum... | [
{
"created": "Wed, 11 Oct 2023 19:04:10 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Oct 2023 18:59:10 GMT",
"version": "v2"
},
{
"created": "Mon, 1 Apr 2024 18:22:43 GMT",
"version": "v3"
}
] | 2024-04-03 | [
[
"Anabalón",
"Andrés",
""
],
[
"Nastase",
"Horatiu",
""
]
] | We show that the d'Alembertian operator with a possible mass term in the AdS soliton and more general confining gravity dual backrounds admits infinitely many different spectra. These can be interpreted as different theories in the infrared and correspond to multitrace deformations of either the Dirichlet or the Neuman... | 12.58523 | 12.974407 | 13.381451 | 12.63948 | 12.885065 | 12.954348 | 13.428099 | 12.185284 | 12.150394 | 14.873099 | 12.369414 | 12.580241 | 12.399221 | 12.241334 | 12.4621 | 12.624307 | 12.623871 | 12.650218 | 12.394188 | 12.60427 | 12.269284 |
1501.01394 | George Savvidy K | George Savvidy | The Gonihedric Paradigm Extensions of the Ising Model | 19 pages, 7 figures, International Conference on Statistical Physics
2014 - SigmaPhi2014, 7-11 July 2014, Rhodes, Greece, references added | null | 10.1142/S0217984915502036 | NRCPS-HE-1-2015 | hep-th cond-mat.stat-mech hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We suggest a generalization of the Feynman path integral to an integral over
random surfaces. The proposed action is proportional to the linear size of the
random surfaces and is called gonihedric. The convergence and the properties of
the partition function are analysed. The model can also be formulated as a spin
sy... | [
{
"created": "Wed, 7 Jan 2015 08:45:18 GMT",
"version": "v1"
},
{
"created": "Mon, 7 Dec 2015 09:30:40 GMT",
"version": "v2"
},
{
"created": "Mon, 12 Dec 2016 19:22:58 GMT",
"version": "v3"
}
] | 2016-12-13 | [
[
"Savvidy",
"George",
""
]
] | We suggest a generalization of the Feynman path integral to an integral over random surfaces. The proposed action is proportional to the linear size of the random surfaces and is called gonihedric. The convergence and the properties of the partition function are analysed. The model can also be formulated as a spin syst... | 10.231849 | 11.135642 | 11.337274 | 10.343449 | 10.777596 | 10.65517 | 11.2025 | 10.326781 | 10.551004 | 11.311737 | 10.594254 | 10.30599 | 10.029663 | 10.181144 | 10.261335 | 10.481315 | 10.288576 | 9.812252 | 10.199783 | 10.497373 | 10.009095 |
hep-th/0211113 | Ergin Sezgin | J. Engquist, E. Sezgin and P. Sundell | Superspace Formulation of 4D Higher Spin Gauge Theory | 24 pp | Nucl.Phys. B664 (2003) 439-456 | 10.1016/S0550-3213(03)00411-5 | null | hep-th | null | Interacting AdS_4 higher spin gauge theories with N \geq 1 supersymmetry so
far have been formulated as constrained systems of differential forms living in
a twistor extension of 4D spacetime. Here we formulate the minimal N=1 theory
in superspace, leaving the internal twistor space intact. Remarkably, the
superspace... | [
{
"created": "Wed, 13 Nov 2002 07:26:34 GMT",
"version": "v1"
}
] | 2010-04-05 | [
[
"Engquist",
"J.",
""
],
[
"Sezgin",
"E.",
""
],
[
"Sundell",
"P.",
""
]
] | Interacting AdS_4 higher spin gauge theories with N \geq 1 supersymmetry so far have been formulated as constrained systems of differential forms living in a twistor extension of 4D spacetime. Here we formulate the minimal N=1 theory in superspace, leaving the internal twistor space intact. Remarkably, the superspace c... | 12.394171 | 10.837208 | 12.392194 | 10.594882 | 10.352234 | 11.319483 | 10.613485 | 11.38036 | 10.385862 | 14.607739 | 9.769594 | 9.922398 | 10.042634 | 10.045333 | 9.847631 | 10.131574 | 9.784219 | 9.997969 | 9.679073 | 11.044447 | 10.03885 |
1010.5789 | Peter Patalong | Dieter Lust, Peter Patalong and Dimitrios Tsimpis | Generalized geometry, calibrations and supersymmetry in diverse
dimensions | 28 pages, 1 table | JHEP 1101:063,2011 | 10.1007/JHEP01(2011)063 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider type II backgrounds of the form R^{1,d-1} x M^{10-d} for even d,
preserving 2^{d/2} real supercharges; for d = 4, 6, 8 this is minimal
supersymmetry in d dimensions, while for d = 2 it is N = (2,0) supersymmetry in
two dimensions. For d = 6 we prove, by explicitly solving the Killing-spinor
equations, tha... | [
{
"created": "Wed, 27 Oct 2010 20:00:12 GMT",
"version": "v1"
}
] | 2011-01-27 | [
[
"Lust",
"Dieter",
""
],
[
"Patalong",
"Peter",
""
],
[
"Tsimpis",
"Dimitrios",
""
]
] | We consider type II backgrounds of the form R^{1,d-1} x M^{10-d} for even d, preserving 2^{d/2} real supercharges; for d = 4, 6, 8 this is minimal supersymmetry in d dimensions, while for d = 2 it is N = (2,0) supersymmetry in two dimensions. For d = 6 we prove, by explicitly solving the Killing-spinor equations, that ... | 7.338549 | 6.798236 | 9.194036 | 6.869365 | 6.836032 | 7.008081 | 7.111403 | 6.505209 | 7.076135 | 9.392724 | 6.884737 | 7.025739 | 7.714825 | 6.999219 | 7.305211 | 6.814355 | 7.107192 | 6.871878 | 7.04184 | 7.589729 | 6.868736 |
2306.00990 | Upamanyu Moitra | Atish Dabholkar, Upamanyu Moitra | Finite Entanglement Entropy in String Theory | 6 pages; two-column format | null | null | null | hep-th gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the one-loop quantum entanglement entropy in ten-dimensional
Type-II string theory using the orbifold method by analytically continuing in
$N$ the genus-one partition function for string orbifolds on
$\mathbb{R}^2/\mathbb{Z}_N$ conical spaces known for all odd integers $N > 1$.
We show that the tachyonic c... | [
{
"created": "Thu, 1 Jun 2023 17:59:59 GMT",
"version": "v1"
}
] | 2023-06-02 | [
[
"Dabholkar",
"Atish",
""
],
[
"Moitra",
"Upamanyu",
""
]
] | We analyze the one-loop quantum entanglement entropy in ten-dimensional Type-II string theory using the orbifold method by analytically continuing in $N$ the genus-one partition function for string orbifolds on $\mathbb{R}^2/\mathbb{Z}_N$ conical spaces known for all odd integers $N > 1$. We show that the tachyonic con... | 7.847994 | 6.670697 | 7.692276 | 6.938012 | 7.062685 | 7.813941 | 7.168683 | 6.459571 | 7.149696 | 8.974417 | 6.812081 | 6.994638 | 7.217122 | 7.221431 | 7.209777 | 7.32964 | 7.373562 | 7.104756 | 7.251377 | 7.626504 | 7.08106 |
1708.07981 | Mahdis Ghodrati | Mahdis Ghodrati | On complexity growth in massive gravity theories, the effects of
chirality and more | 33 pages, 3 figures | Phys. Rev. D 96, 106020 (2017) | 10.1103/PhysRevD.96.106020 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | To study the effect of parity-violation on the rate of complexity growth, by
using "Complexity=Action" conjecture, we find the complexity growth rates in
different solutions of the chiral theory of Topologically Massive Gravity (TMG)
and parity-preserving theory of New Massive Gravity (NMG). Using the results,
one ca... | [
{
"created": "Sat, 26 Aug 2017 14:51:18 GMT",
"version": "v1"
}
] | 2017-12-01 | [
[
"Ghodrati",
"Mahdis",
""
]
] | To study the effect of parity-violation on the rate of complexity growth, by using "Complexity=Action" conjecture, we find the complexity growth rates in different solutions of the chiral theory of Topologically Massive Gravity (TMG) and parity-preserving theory of New Massive Gravity (NMG). Using the results, one can ... | 11.520386 | 10.543588 | 11.588438 | 9.65103 | 10.539286 | 10.640695 | 11.302933 | 10.659427 | 10.887882 | 12.023458 | 10.323261 | 10.036392 | 10.780623 | 10.267561 | 10.179896 | 10.540755 | 10.607753 | 10.107717 | 9.867432 | 10.874782 | 9.663905 |
hep-th/0210139 | Mohammad Reza Garousi | M.R. Garousi, G.R. Maktabdaran | Excited D-brane decay in Cubic String Field Theory and in Bosonic String
Theory | 19 pages, Latex, v3; references added, some words about contact terms
are added | Nucl.Phys. B651 (2003) 26-44 | 10.1016/S0550-3213(02)01128-8 | IPM/2002/051 | hep-th | null | In the cubic string field theory, using the gauge invariant operators
corresponding to the on-shell closed string vertex operators, we have
explicitly evaluated the decay amplitudes of two open string tachyons or gauge
fields to one closed string tachyon or graviton up to level two. We then
evaluated the same amplitu... | [
{
"created": "Tue, 15 Oct 2002 16:11:14 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Oct 2002 13:07:26 GMT",
"version": "v2"
},
{
"created": "Sun, 1 Dec 2002 07:46:53 GMT",
"version": "v3"
}
] | 2010-04-05 | [
[
"Garousi",
"M. R.",
""
],
[
"Maktabdaran",
"G. R.",
""
]
] | In the cubic string field theory, using the gauge invariant operators corresponding to the on-shell closed string vertex operators, we have explicitly evaluated the decay amplitudes of two open string tachyons or gauge fields to one closed string tachyon or graviton up to level two. We then evaluated the same amplitude... | 6.988616 | 6.19005 | 7.078411 | 6.164797 | 6.324186 | 5.997109 | 6.011227 | 6.440474 | 5.86482 | 8.512909 | 6.334455 | 6.326205 | 6.78792 | 6.315855 | 6.486163 | 6.275248 | 6.386459 | 6.331953 | 6.289474 | 6.536679 | 6.180684 |
hep-th/9211092 | null | Zhu Yang | Asymptotic Freedom and Dirichlet String Theory, UR-1288, ER-40685-737 | 12 pages | null | null | null | hep-th hep-ph | null | Fixed angle scattering at high energy in a string theory with boundaries
satisfying Dirichlet conditions (Dirichlet strings) in $D=4$ is shown to have
logarithmic dependence on energy, in addition to the power-like behavior known
before. High temperature free energy also depends logarithmically on
temperature. Such a... | [
{
"created": "Sat, 21 Nov 1992 18:24:00 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Yang",
"Zhu",
""
]
] | Fixed angle scattering at high energy in a string theory with boundaries satisfying Dirichlet conditions (Dirichlet strings) in $D=4$ is shown to have logarithmic dependence on energy, in addition to the power-like behavior known before. High temperature free energy also depends logarithmically on temperature. Such a r... | 13.904465 | 11.772844 | 12.040645 | 11.471363 | 12.161083 | 13.56575 | 12.292298 | 11.676148 | 12.182866 | 12.817987 | 11.816766 | 11.488304 | 12.076297 | 11.409534 | 11.623616 | 11.468554 | 11.896732 | 11.455718 | 11.374453 | 12.004089 | 12.152591 |
hep-th/0012123 | Emanuele Raineri | Shahn Majid and E. Raineri | Electromagnetism and Gauge Theory on the Permutation Group $S_3$ | 28 pages, LaTex as revised March 2001 -- expanded remarks in last
section on the quantum theory, but no sig. changes | J.Geom.Phys. 44 (2002) 129-155 | 10.1016/S0393-0440(02)00052-9 | null | hep-th math.QA | null | Using noncommutative geometry we do U(1) gauge theory on the permutation
group $S_3$. Unlike usual lattice gauge theories the use of a nonAbelian group
here as spacetime corresponds to a background Riemannian curvature. In this
background we solve spin 0, 1/2 and spin 1 equations of motion, including the
spin 1 or `p... | [
{
"created": "Thu, 14 Dec 2000 17:01:11 GMT",
"version": "v1"
},
{
"created": "Sun, 17 Dec 2000 20:37:26 GMT",
"version": "v2"
},
{
"created": "Tue, 11 Sep 2001 18:44:14 GMT",
"version": "v3"
}
] | 2015-06-25 | [
[
"Majid",
"Shahn",
""
],
[
"Raineri",
"E.",
""
]
] | Using noncommutative geometry we do U(1) gauge theory on the permutation group $S_3$. Unlike usual lattice gauge theories the use of a nonAbelian group here as spacetime corresponds to a background Riemannian curvature. In this background we solve spin 0, 1/2 and spin 1 equations of motion, including the spin 1 or `pho... | 10.065681 | 9.841351 | 9.813588 | 9.430801 | 10.132046 | 10.538365 | 10.211602 | 9.804464 | 9.487688 | 10.518739 | 9.147597 | 9.486547 | 9.833234 | 9.440047 | 9.275683 | 9.944399 | 9.766022 | 9.562097 | 9.228244 | 9.374383 | 9.513135 |
hep-th/0208033 | Chiang-Mei Chen | Chiang-Mei Chen, T. Harko, W.F. Kao and M.K. Mak | Rotational Perturbations of High Density Matter in the Brane Cosmology | final version to appear in JCAP | JCAP 0311:005,2003 | 10.1088/1475-7516/2003/11/005 | null | hep-th | null | We consider the evolution of small rotational perturbations, with azimuthal
symmetry, of the brane-world cosmological models. The equations describing the
temporal, radial, and angular dependence of the perturbations are derived by
taking into account the effects of both scalar and tensor parts of the dark
energy ter... | [
{
"created": "Mon, 5 Aug 2002 03:18:10 GMT",
"version": "v1"
},
{
"created": "Mon, 30 Dec 2002 03:20:11 GMT",
"version": "v2"
},
{
"created": "Thu, 16 Oct 2003 03:07:22 GMT",
"version": "v3"
}
] | 2010-11-19 | [
[
"Chen",
"Chiang-Mei",
""
],
[
"Harko",
"T.",
""
],
[
"Kao",
"W. F.",
""
],
[
"Mak",
"M. K.",
""
]
] | We consider the evolution of small rotational perturbations, with azimuthal symmetry, of the brane-world cosmological models. The equations describing the temporal, radial, and angular dependence of the perturbations are derived by taking into account the effects of both scalar and tensor parts of the dark energy term ... | 8.782624 | 9.600682 | 8.474136 | 8.818974 | 9.051657 | 9.566833 | 9.224159 | 8.205465 | 8.897544 | 9.115952 | 8.997259 | 8.647937 | 8.258953 | 8.33518 | 8.426478 | 8.480043 | 8.627914 | 8.17748 | 8.541316 | 8.614601 | 8.623817 |
1508.02188 | Peter Horvathy | M. Elbistan, C. Duval, P. A. Horvathy, P.-M. Zhang | Helicity of spin-extended chiral particles | Published version, slightly extended. 18 pages, 4 figures | Phys. Lett. A 380, 1677-1683 (2016) | 10.1016/j.physleta.2016.03.016 | null | hep-th cond-mat.other hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The helicity of a free massless relativistic particle, $\chi^o={\bf s}.{\bf
p}/|{\bf p}|$, is generalized, for a particle in an electromagnetic field, to
$\chi={\bf s}.{\bf p}/{\cal E}$, where ${\cal E}$ is the modified kinetic
energy. Both $\chi^o$ and $\chi$ coincide and are conserved for minimal
coupling (gyromagn... | [
{
"created": "Mon, 10 Aug 2015 09:47:45 GMT",
"version": "v1"
},
{
"created": "Mon, 21 Sep 2015 07:00:35 GMT",
"version": "v2"
},
{
"created": "Fri, 19 Feb 2016 01:34:26 GMT",
"version": "v3"
},
{
"created": "Tue, 8 Mar 2016 15:06:47 GMT",
"version": "v4"
},
{
"cr... | 2016-04-05 | [
[
"Elbistan",
"M.",
""
],
[
"Duval",
"C.",
""
],
[
"Horvathy",
"P. A.",
""
],
[
"Zhang",
"P. -M.",
""
]
] | The helicity of a free massless relativistic particle, $\chi^o={\bf s}.{\bf p}/|{\bf p}|$, is generalized, for a particle in an electromagnetic field, to $\chi={\bf s}.{\bf p}/{\cal E}$, where ${\cal E}$ is the modified kinetic energy. Both $\chi^o$ and $\chi$ coincide and are conserved for minimal coupling (gyromagnet... | 6.386833 | 6.344816 | 6.340192 | 6.044465 | 6.468952 | 6.257769 | 6.472502 | 6.411665 | 6.119026 | 6.423709 | 6.180865 | 6.341788 | 5.997657 | 6.19533 | 6.141188 | 5.993743 | 6.112278 | 6.05343 | 6.112618 | 6.250655 | 6.194798 |
hep-th/9502028 | Gennadi Lykasov | G.I.Lykasov, M.N.Sergeenko | Semihard Hadron Processes and Quark-gluon String Model | resubmitted as hep-ph/9502316. Removed from hep-th. | null | null | null | hep-th | null | Resubmitted as hep-ph/9502316. Removed from hep-th. Incorrigibly inept
submitter publicly excoriated.
| [
{
"created": "Fri, 3 Feb 1995 18:25:44 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Lykasov",
"G. I.",
""
],
[
"Sergeenko",
"M. N.",
""
]
] | Resubmitted as hep-ph/9502316. Removed from hep-th. Incorrigibly inept submitter publicly excoriated. | 51.789848 | 49.431152 | 48.078285 | 35.163723 | 45.196056 | 62.926342 | 47.803406 | 46.635227 | 44.24395 | 51.336044 | 60.169357 | 48.77919 | 44.479351 | 40.642269 | 41.786049 | 42.978008 | 40.906555 | 46.362309 | 44.223373 | 40.536964 | 48.123665 |
hep-th/0209193 | Christopher Pope | M. Cvetic, H. Lu, C.N. Pope and K.S. Stelle | Linearly-realised Worldsheet Supersymmetry in pp-wave Background | Latex, 35 pages | Nucl.Phys.B662:89-119,2003 | 10.1016/S0550-3213(03)00263-3 | null | hep-th | null | We study the linearly-realised worldsheet supersymmetries in the ``massive''
type II light-cone actions for pp-wave backgrounds. The pp-waves have have
16+N_sup Killing spinors, comprising 16 ``standard'' Killing spinors that occur
in any wave background, plus N_sup ``supernumerary'' Killing spinors (0\le
N_sup \le 1... | [
{
"created": "Tue, 24 Sep 2002 18:53:11 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cvetic",
"M.",
""
],
[
"Lu",
"H.",
""
],
[
"Pope",
"C. N.",
""
],
[
"Stelle",
"K. S.",
""
]
] | We study the linearly-realised worldsheet supersymmetries in the ``massive'' type II light-cone actions for pp-wave backgrounds. The pp-waves have have 16+N_sup Killing spinors, comprising 16 ``standard'' Killing spinors that occur in any wave background, plus N_sup ``supernumerary'' Killing spinors (0\le N_sup \le 16)... | 7.38776 | 7.066358 | 8.273241 | 7.247381 | 7.152694 | 7.318543 | 7.53662 | 7.060362 | 7.015091 | 8.905296 | 7.033502 | 7.102887 | 7.162888 | 6.939565 | 6.797193 | 6.945855 | 6.818478 | 7.016713 | 6.940539 | 7.445414 | 6.696522 |
hep-th/9611050 | Joe Polchinski | Joseph Polchinski | TASI Lectures on D-Branes | 63 Pages, LaTeX, 13 epsf figures, TASI96(d-branes) Small corrections
and clarifications. More complete list of early references in section 1.1 | null | null | NSF-ITP-96-145 | hep-th | null | This is an introduction to the properties of D-branes, topological defects in
string theory on which string endpoints can live. D-branes provide a simple
description of various nonperturbative objects required by string duality, and
give new insight into the quantum mechanics of black holes and the nature of
spacetim... | [
{
"created": "Fri, 8 Nov 1996 01:16:40 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Apr 1997 17:20:40 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Polchinski",
"Joseph",
""
]
] | This is an introduction to the properties of D-branes, topological defects in string theory on which string endpoints can live. D-branes provide a simple description of various nonperturbative objects required by string duality, and give new insight into the quantum mechanics of black holes and the nature of spacetime ... | 7.531269 | 9.810993 | 8.471775 | 7.615126 | 8.809203 | 7.817927 | 8.353863 | 9.018385 | 8.050009 | 8.846373 | 8.180644 | 7.839659 | 8.733534 | 7.389129 | 7.781145 | 7.860349 | 7.788771 | 7.474802 | 7.705402 | 8.345721 | 7.715682 |
2406.13643 | Slobodan Radosevic | Slobodan Rado\v{s}evi\'c | Geometry of Classical Nambu-Goldstone Fields | 20 pages | null | null | null | hep-th cond-mat.str-el hep-ph | http://creativecommons.org/licenses/by/4.0/ | A coordinate-free formulation of first order effective field theory, in which
Nambu-Goldstone fields are described as sections on associated bundle, is
presented. This construction, which is based only on symmetry considerations,
allows for a direct derivation of number and types of Nambu-Goldstone fields in
a classi... | [
{
"created": "Wed, 19 Jun 2024 15:45:43 GMT",
"version": "v1"
}
] | 2024-06-21 | [
[
"Radošević",
"Slobodan",
""
]
] | A coordinate-free formulation of first order effective field theory, in which Nambu-Goldstone fields are described as sections on associated bundle, is presented. This construction, which is based only on symmetry considerations, allows for a direct derivation of number and types of Nambu-Goldstone fields in a classica... | 11.843976 | 9.333399 | 9.923462 | 10.010162 | 10.304354 | 11.553323 | 10.702192 | 9.700167 | 10.829364 | 11.218472 | 9.651073 | 9.821871 | 10.511122 | 9.99189 | 10.183125 | 9.906376 | 10.123316 | 10.101453 | 10.124052 | 10.228668 | 9.972417 |
hep-th/9910111 | Mihail Mihailescu | Mihail Mihailescu | Correlation functions for chiral primaries in D=6 Supergravity on $AdS_3
\times S^3$ | 15 pages, harvmac big | JHEP 0002 (2000) 007 | 10.1088/1126-6708/2000/02/007 | null | hep-th | null | Six dimensional supergravities on $ADS_3 \times S^3$ present interest due to
the role they play in the $AdS/CFT$ correspondence. The correspondence in this
case states the equivalence between supergravity on the given background and a
still unknown conformal field theory. The conformal field theory in question is
exp... | [
{
"created": "Thu, 14 Oct 1999 22:52:23 GMT",
"version": "v1"
}
] | 2009-10-31 | [
[
"Mihailescu",
"Mihail",
""
]
] | Six dimensional supergravities on $ADS_3 \times S^3$ present interest due to the role they play in the $AdS/CFT$ correspondence. The correspondence in this case states the equivalence between supergravity on the given background and a still unknown conformal field theory. The conformal field theory in question is expec... | 9.285787 | 9.298864 | 9.774757 | 9.102521 | 9.683138 | 9.5418 | 9.647003 | 9.287675 | 9.157619 | 10.457377 | 9.229923 | 8.942926 | 9.142192 | 8.690406 | 8.570002 | 8.63932 | 8.730257 | 8.692578 | 8.66583 | 9.032794 | 8.739082 |
1809.08255 | Jorge Fern\'andez-Pend\'as | Christian Copetti and Jorge Fern\'andez-Pend\'as | Higher spin vortical Zilches from Kubo formulae | 6 pages + 3 pages of supplemental materials | Phys. Rev. D 98, 105008 (2018) | 10.1103/PhysRevD.98.105008 | IFT-UAM/CSIC-18-96 | hep-th cond-mat.other | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We compute thermal one point functions in Maxwell's theory sourced by
vorticity for the Zilch and its higher spin extensions via the Kubo formalism.
This leads to a generalization of the recent results of
\citep{Chernodub:2018era} to any spin and their value suggests a relation with
possible anomalies for the higher ... | [
{
"created": "Fri, 21 Sep 2018 18:00:57 GMT",
"version": "v1"
}
] | 2018-11-28 | [
[
"Copetti",
"Christian",
""
],
[
"Fernández-Pendás",
"Jorge",
""
]
] | We compute thermal one point functions in Maxwell's theory sourced by vorticity for the Zilch and its higher spin extensions via the Kubo formalism. This leads to a generalization of the recent results of \citep{Chernodub:2018era} to any spin and their value suggests a relation with possible anomalies for the higher sp... | 23.384869 | 20.792477 | 25.035318 | 22.585884 | 24.969389 | 27.04871 | 25.193214 | 22.949821 | 20.61282 | 25.654924 | 22.532969 | 21.020689 | 22.036612 | 19.483599 | 20.585873 | 20.690479 | 20.342218 | 19.625856 | 21.274288 | 20.419985 | 20.635489 |
1709.00637 | Fabio Scardigli | Gaetano Lambiase and Fabio Scardigli | Lorentz violation and generalized uncertainty principle | 9 pages, no figures | Phys. Rev. D 97, 075003 (2018) | 10.1103/PhysRevD.97.075003 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Investigations on possible violation of Lorentz invariance have been widely
pursued in the last decades, both from theoretical and experimental sides. A
comprehensive framework to formulate the problem is the standard model
extension (SME) proposed by A.Kostelecky, where violation of Lorentz invariance
is encoded int... | [
{
"created": "Sat, 2 Sep 2017 21:50:49 GMT",
"version": "v1"
}
] | 2018-04-11 | [
[
"Lambiase",
"Gaetano",
""
],
[
"Scardigli",
"Fabio",
""
]
] | Investigations on possible violation of Lorentz invariance have been widely pursued in the last decades, both from theoretical and experimental sides. A comprehensive framework to formulate the problem is the standard model extension (SME) proposed by A.Kostelecky, where violation of Lorentz invariance is encoded into ... | 5.018346 | 5.19199 | 4.848528 | 4.711562 | 5.107596 | 5.025729 | 5.364398 | 4.746186 | 4.885579 | 5.240318 | 4.979321 | 4.942096 | 4.747975 | 4.786106 | 4.856475 | 4.891408 | 4.927073 | 4.75584 | 4.754242 | 4.877077 | 4.833184 |
hep-th/9410064 | Vadim Zeitlin | Vadim Zeitlin | QED$_{2+1}$ with Nonzero Fermion Density and Quantum Hall Effect | 8 pages, LaTeX; FIAN/TD/94-09 | Phys. Lett. B352 (1995) 422 | 10.1016/0370-2693(95)00488-7 | null | hep-th cond-mat | null | A general expression for the conductivity in the QED$_{2+1}$ with nonzero
fermion density in the uniform magnetic field is derived. It is shown that the
conductivity is entirely determined by the Chern-Simons coefficient:
$\sigma_{ij}=\varepsilon_{ij}~{\cal C}$ and is a step-function of the chemical
potential and the... | [
{
"created": "Mon, 10 Oct 1994 13:58:51 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Zeitlin",
"Vadim",
""
]
] | A general expression for the conductivity in the QED$_{2+1}$ with nonzero fermion density in the uniform magnetic field is derived. It is shown that the conductivity is entirely determined by the Chern-Simons coefficient: $\sigma_{ij}=\varepsilon_{ij}~{\cal C}$ and is a step-function of the chemical potential and the m... | 7.493346 | 6.443751 | 7.328106 | 6.249684 | 6.332815 | 7.626663 | 7.06882 | 7.08092 | 6.660312 | 7.082004 | 6.958862 | 6.626445 | 7.005771 | 6.345155 | 6.319232 | 6.778354 | 6.527828 | 6.784055 | 6.564302 | 7.015829 | 6.436023 |
hep-th/9711077 | A. Sagnotti | Fabio Riccioni and Augusto Sagnotti (U. Roma "Tor Vergata") | Some Properties of Tensor Multiplets in Six-Dimensional Supergravity | 6 pages, LateX. Contribution to the Proceedings of "String Duality,
II", Trieste, april 1997 | Nucl.Phys.Proc.Suppl. 67 (1998) 68-73 | 10.1016/S0920-5632(98)00121-2 | ROM2F-97/38 | hep-th | null | We review some results on the complete coupling between tensor and vector
multiplets in six-dimensional $(1,0)$ supergravity.
| [
{
"created": "Tue, 11 Nov 1997 16:40:37 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Riccioni",
"Fabio",
"",
"U. Roma \"Tor Vergata\""
],
[
"Sagnotti",
"Augusto",
"",
"U. Roma \"Tor Vergata\""
]
] | We review some results on the complete coupling between tensor and vector multiplets in six-dimensional $(1,0)$ supergravity. | 18.426603 | 7.585536 | 16.835732 | 8.514708 | 8.153845 | 8.153179 | 7.686114 | 9.121887 | 8.531728 | 15.102892 | 7.799378 | 9.196279 | 12.538478 | 10.167634 | 9.496743 | 9.919484 | 9.158279 | 9.824354 | 9.480057 | 12.028533 | 8.915751 |
hep-th/9904201 | Marco Bochicchio | Marco Bochicchio | The confining branch of QCD | 8 pages, latex, no figures, a misprint corrected | null | null | ROME 1250/99 | hep-th | null | We show that, as a consequence of a physical interpretation based on the
Abelian projection and on the QCD string, four-dimensional QCD confines the
electric flux if and only if the functional integral in the fiberwise-dual
variables admits a hyper-Kahler reduction under the action of the gauge group.
| [
{
"created": "Wed, 28 Apr 1999 23:39:50 GMT",
"version": "v1"
},
{
"created": "Mon, 24 May 1999 18:41:50 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Bochicchio",
"Marco",
""
]
] | We show that, as a consequence of a physical interpretation based on the Abelian projection and on the QCD string, four-dimensional QCD confines the electric flux if and only if the functional integral in the fiberwise-dual variables admits a hyper-Kahler reduction under the action of the gauge group. | 17.952175 | 16.897655 | 19.478266 | 15.929865 | 16.029503 | 17.489353 | 18.746256 | 18.125654 | 18.177809 | 21.57881 | 17.232304 | 16.07312 | 16.412155 | 16.348232 | 16.065479 | 15.769807 | 16.977318 | 15.835126 | 16.191984 | 16.646641 | 16.053328 |
0709.2822 | Roberto D. Mota Esteves | Ruben Cordero and Roberto D. Mota | Soliton Stability in a Generalized Sine-Gordon Potential | null | Int.J.Theor.Phys.43:2215-2222,2004 | 10.1023/B:IJTP.0000049020.06344.54 | null | hep-th | null | We study stability of a generalized sine-Gordon model with two coupled scalar
fields in two dimensions. Topological soliton solutions are found from the
first-order equations that solve the equations of motion. The perturbation
equations can be cast in terms of a Schrodinger-like operators for fluctuations
and their ... | [
{
"created": "Tue, 18 Sep 2007 13:29:25 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Cordero",
"Ruben",
""
],
[
"Mota",
"Roberto D.",
""
]
] | We study stability of a generalized sine-Gordon model with two coupled scalar fields in two dimensions. Topological soliton solutions are found from the first-order equations that solve the equations of motion. The perturbation equations can be cast in terms of a Schrodinger-like operators for fluctuations and their sp... | 13.239696 | 8.705949 | 12.068902 | 10.269339 | 10.51608 | 10.302241 | 9.67194 | 9.960225 | 9.760659 | 11.52765 | 9.528756 | 10.151626 | 10.801484 | 10.673607 | 10.924978 | 10.741969 | 10.968141 | 11.056408 | 10.536542 | 10.834949 | 10.466322 |
1202.1736 | Carlos Andres Cardona Giraldo | Carlos A. Cardona | Comments on Correlation Functions of Large Spin Operators and Null
Polygonal Wilson Loops | 16+3 pages, 3 figures. Computation in section 4.1 has been clarified.
Some comments on the vertex contributions has been added in section 4.2. Some
other minor corrections. Version to appear in Nucl. Phys. B | null | 10.1016/j.nuclphysb.2012.09.017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the relation between correlation functions of twist-two large spin
operators and expectation values of Wilson loops along light-like trajectories.
After presenting some heuristic field theoretical arguments suggesting this
relation, we compute the divergent part of the correlator in the limit of large
't H... | [
{
"created": "Wed, 8 Feb 2012 15:26:41 GMT",
"version": "v1"
},
{
"created": "Thu, 27 Sep 2012 20:28:18 GMT",
"version": "v2"
}
] | 2015-06-04 | [
[
"Cardona",
"Carlos A.",
""
]
] | We discuss the relation between correlation functions of twist-two large spin operators and expectation values of Wilson loops along light-like trajectories. After presenting some heuristic field theoretical arguments suggesting this relation, we compute the divergent part of the correlator in the limit of large 't Hoo... | 9.313459 | 10.704734 | 10.685842 | 10.241076 | 10.979009 | 10.72503 | 10.433457 | 11.238439 | 9.98657 | 12.605122 | 9.554604 | 10.324122 | 10.122191 | 9.442992 | 9.495903 | 9.795463 | 9.646943 | 10.057068 | 9.471057 | 9.929565 | 9.501114 |
1911.07276 | Stefan Hohenegger | Brice Bastian, Stefan Hohenegger | Symmetries in A-Type Little String Theories, Part I | 33 pages | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyse the symmetries of a class of A-type little string theories that
are engineered by $N$ parallel M5-branes with M2-branes stretched between them.
This paper deals with the so-called reduced free energy, which only receives
contributions from the subset of the BPS states that carry the same charges
under all ... | [
{
"created": "Sun, 17 Nov 2019 16:35:36 GMT",
"version": "v1"
}
] | 2019-11-19 | [
[
"Bastian",
"Brice",
""
],
[
"Hohenegger",
"Stefan",
""
]
] | We analyse the symmetries of a class of A-type little string theories that are engineered by $N$ parallel M5-branes with M2-branes stretched between them. This paper deals with the so-called reduced free energy, which only receives contributions from the subset of the BPS states that carry the same charges under all th... | 8.163675 | 7.528538 | 9.34017 | 7.478757 | 8.372073 | 8.024388 | 7.743022 | 7.295156 | 7.408074 | 10.289272 | 7.37199 | 7.567454 | 8.291861 | 7.622737 | 7.817125 | 7.700401 | 7.588727 | 7.443599 | 7.784594 | 8.40124 | 7.613903 |
2205.06273 | Lars Aalsma | Lars Aalsma and Gary Shiu | From Rotating to Charged Black Holes and Back Again | 17+2 pages | null | 10.1007/JHEP11(2022)161 | null | hep-th gr-qc hep-ph | http://creativecommons.org/licenses/by/4.0/ | The mild form of the Weak Gravity Conjecture (WGC) requires higher derivative
corrections to extremal charged black holes to increase their charge-to-mass
ratio. This allows decay via emission of a smaller extremal black hole. In this
paper, we investigate if similar constraints hold for extremal rotating black
holes... | [
{
"created": "Thu, 12 May 2022 18:00:01 GMT",
"version": "v1"
}
] | 2022-12-21 | [
[
"Aalsma",
"Lars",
""
],
[
"Shiu",
"Gary",
""
]
] | The mild form of the Weak Gravity Conjecture (WGC) requires higher derivative corrections to extremal charged black holes to increase their charge-to-mass ratio. This allows decay via emission of a smaller extremal black hole. In this paper, we investigate if similar constraints hold for extremal rotating black holes. ... | 7.201289 | 6.68154 | 7.414905 | 6.446783 | 6.321347 | 6.732298 | 6.550225 | 6.65835 | 6.783011 | 7.396804 | 6.431479 | 6.852403 | 7.076874 | 6.634332 | 6.658524 | 6.83856 | 6.697766 | 6.756711 | 6.850643 | 6.937544 | 6.967407 |
1707.09452 | E. Aldo Arroyo | E. Aldo Arroyo, A. Fernandes-Silva, R. Szitas | Numerical solution of open string field theory in Schnabl gauge | 37 pages, 9 figures, some typos corrected | null | 10.1007/JHEP01(2018)007 | CCNH-UFABC 2017 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Using traditional Virasoro $L_0$ level-truncation computations, we evaluate
the open bosonic string field theory action up to level $(10,30)$. Extremizing
this level-truncated potential, we construct a numerical solution for tachyon
condensation in Schnabl gauge. We find that the energy associated to the
numerical so... | [
{
"created": "Sat, 29 Jul 2017 02:27:14 GMT",
"version": "v1"
},
{
"created": "Sat, 16 Sep 2017 01:52:47 GMT",
"version": "v2"
},
{
"created": "Tue, 19 Sep 2017 10:27:36 GMT",
"version": "v3"
},
{
"created": "Wed, 22 Nov 2017 16:20:53 GMT",
"version": "v4"
}
] | 2018-01-09 | [
[
"Arroyo",
"E. Aldo",
""
],
[
"Fernandes-Silva",
"A.",
""
],
[
"Szitas",
"R.",
""
]
] | Using traditional Virasoro $L_0$ level-truncation computations, we evaluate the open bosonic string field theory action up to level $(10,30)$. Extremizing this level-truncated potential, we construct a numerical solution for tachyon condensation in Schnabl gauge. We find that the energy associated to the numerical solu... | 6.427749 | 5.602764 | 7.388212 | 5.84128 | 6.317168 | 6.075595 | 5.592155 | 5.980662 | 5.528845 | 7.355135 | 5.921072 | 5.853153 | 6.319002 | 5.916626 | 6.1909 | 5.882679 | 5.836829 | 6.028692 | 5.876687 | 6.291555 | 6.040745 |
1701.00467 | Mikhail Shifman | Mikhail Shifman, Arkady Vainshtein | (In)dependence of Theta in the Higgs Regime without Axions | 14 pp, 1 figure | Mod. Phys. Lett. A, Vol. 32, No. 14 (2017) 1750084 | 10.1142/S0217732317500845 | FTPI-MINN-16/36, UMN-TH-3616/16 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We revisit the issue of the vacuum angle theta dependence in weakly coupled
(Higgsed) Yang-Mills theories. Two most popular mechanisms for eliminating
physical theta dependence are massless quarks and axions. Anselm and Johansen
noted that the vacuum angle theta(EW), associated with the electroweak SU(2) in
the Glash... | [
{
"created": "Mon, 2 Jan 2017 17:55:35 GMT",
"version": "v1"
}
] | 2017-04-26 | [
[
"Shifman",
"Mikhail",
""
],
[
"Vainshtein",
"Arkady",
""
]
] | We revisit the issue of the vacuum angle theta dependence in weakly coupled (Higgsed) Yang-Mills theories. Two most popular mechanisms for eliminating physical theta dependence are massless quarks and axions. Anselm and Johansen noted that the vacuum angle theta(EW), associated with the electroweak SU(2) in the Glashow... | 9.067087 | 10.591918 | 9.109875 | 9.421601 | 10.752039 | 10.733871 | 9.954798 | 10.677457 | 9.258992 | 9.902746 | 10.038165 | 9.121541 | 9.166423 | 8.943562 | 9.101976 | 9.546491 | 9.477095 | 9.131959 | 9.165649 | 9.235519 | 9.313293 |
1701.00496 | Daniel Kapec | Temple He, Daniel Kapec, Ana-Maria Raclariu, Andrew Strominger | Loop-Corrected Virasoro Symmetry of 4D Quantum Gravity | 12 pages | JHEP 1708, 050 (2017) | 10.1007/JHEP08(2017)050 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently a boundary energy-momentum tensor $T_{zz}$ has been constructed from
the soft graviton operator for any 4D quantum theory of gravity in
asymptotically flat space. Up to an "anomaly" which is one-loop exact, $T_{zz}$
generates a Virasoro action on the 2D celestial sphere at null infinity. Here
we show by expl... | [
{
"created": "Mon, 2 Jan 2017 19:00:25 GMT",
"version": "v1"
}
] | 2017-11-17 | [
[
"He",
"Temple",
""
],
[
"Kapec",
"Daniel",
""
],
[
"Raclariu",
"Ana-Maria",
""
],
[
"Strominger",
"Andrew",
""
]
] | Recently a boundary energy-momentum tensor $T_{zz}$ has been constructed from the soft graviton operator for any 4D quantum theory of gravity in asymptotically flat space. Up to an "anomaly" which is one-loop exact, $T_{zz}$ generates a Virasoro action on the 2D celestial sphere at null infinity. Here we show by explic... | 8.186261 | 7.461101 | 8.528751 | 7.244433 | 8.483251 | 7.892191 | 7.249729 | 8.026937 | 7.342693 | 9.205824 | 7.718757 | 7.579646 | 8.080738 | 7.284478 | 7.46735 | 7.752834 | 7.937488 | 7.696506 | 7.51475 | 8.17043 | 7.411803 |
1210.4740 | I-Sheng Yang | I-Sheng Yang | Recovering the Negative Mode for Type B Coleman-de Luccia Instantons | version 3, 18 pages, 6 figures, changed the title to follow the
terminology of earlier works and expanded appendix to address the comments
from Brown, Freivogel, Weinberg and Xiao | null | 10.1103/PhysRevD.87.084026 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The usual (type A) thin-wall Coleman-de Luccia instanton is made by a
bigger-than-half sphere of the false vacuum and a smaller-than-half sphere of
the true vacuum. It has a the standard O(4) symmetric negative mode associated
with changing the size of false vacuum region. On the other hand, the type B
instanton, mad... | [
{
"created": "Wed, 17 Oct 2012 13:44:42 GMT",
"version": "v1"
},
{
"created": "Tue, 23 Oct 2012 13:05:15 GMT",
"version": "v2"
},
{
"created": "Thu, 28 Feb 2013 10:44:43 GMT",
"version": "v3"
}
] | 2013-04-17 | [
[
"Yang",
"I-Sheng",
""
]
] | The usual (type A) thin-wall Coleman-de Luccia instanton is made by a bigger-than-half sphere of the false vacuum and a smaller-than-half sphere of the true vacuum. It has a the standard O(4) symmetric negative mode associated with changing the size of false vacuum region. On the other hand, the type B instanton, made ... | 15.446125 | 13.882253 | 14.170922 | 12.601266 | 14.232554 | 13.97626 | 14.287901 | 13.001032 | 12.506588 | 14.056599 | 13.566598 | 12.967629 | 12.471958 | 12.224137 | 12.96843 | 12.774994 | 13.07365 | 12.575583 | 12.32097 | 12.490809 | 13.01089 |
hep-th/9609166 | null | F.A.Lunev | Pure bosonic worldline path integral representation for fermionic
determinants, non-Abelian Stokes theorem, and quasiclassical approximation in
QCD | LaTeX, 49 pages | Nucl.Phys. B494 (1997) 433-470 | 10.1016/S0550-3213(97)00154-5 | null | hep-th hep-lat | null | Simple bosonic path integral representation for path ordered exponent is
derived. This representation is used, at first, to obtain new variant of
non-Abelian Stokes theorem. Then new pure bosonic worldline path integral
representations for fermionic determinant and Green functions are presented.
Finally, applying sta... | [
{
"created": "Thu, 19 Sep 1996 10:47:25 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Lunev",
"F. A.",
""
]
] | Simple bosonic path integral representation for path ordered exponent is derived. This representation is used, at first, to obtain new variant of non-Abelian Stokes theorem. Then new pure bosonic worldline path integral representations for fermionic determinant and Green functions are presented. Finally, applying stati... | 19.322815 | 14.491017 | 16.690769 | 13.573822 | 15.191405 | 15.121551 | 16.21867 | 14.387832 | 14.075761 | 17.682577 | 14.702897 | 14.633224 | 15.045836 | 13.989154 | 14.020975 | 14.419676 | 14.588378 | 14.113754 | 14.366463 | 15.306495 | 14.571258 |
1112.4382 | Semyon Klevtsov | Frank Ferrari, Semyon Klevtsov and Steve Zelditch | Simple matrix models for random Bergman metrics | 23 pages, IOP Latex style, diastatic function Eq. (22) and contact
terms in Eqs. (76, 95) corrected, typos fixed. Accepted to JSTAT | J. Stat. Mech. (2012) P04012 | 10.1088/1742-5468/2012/04/P04012 | null | hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Recently, the authors have proposed a new approach to the theory of random
metrics, making an explicit link between probability measures on the space of
metrics on a Kahler manifold and random matrix models. We consider simple
examples of such models and compute the one and two-point functions of the
metric. These ge... | [
{
"created": "Mon, 19 Dec 2011 16:03:28 GMT",
"version": "v1"
},
{
"created": "Mon, 23 Apr 2012 11:58:49 GMT",
"version": "v2"
}
] | 2012-04-26 | [
[
"Ferrari",
"Frank",
""
],
[
"Klevtsov",
"Semyon",
""
],
[
"Zelditch",
"Steve",
""
]
] | Recently, the authors have proposed a new approach to the theory of random metrics, making an explicit link between probability measures on the space of metrics on a Kahler manifold and random matrix models. We consider simple examples of such models and compute the one and two-point functions of the metric. These geom... | 11.516063 | 11.001819 | 11.174705 | 10.143693 | 10.713114 | 10.807152 | 11.109972 | 10.541989 | 10.767145 | 12.89509 | 10.799496 | 10.185122 | 10.603643 | 10.688509 | 10.341802 | 10.289014 | 10.10277 | 10.281409 | 10.495255 | 10.681147 | 10.479101 |
hep-th/0611304 | Romuald A. Janik | Dongsu Bak, Romuald A. Janik | From static to evolving geometries -- R-charged hydrodynamics from
supergravity | 15 pages, no figures | Phys.Lett.B645:303-308,2007 | 10.1016/j.physletb.2006.12.049 | null | hep-th gr-qc hep-ph | null | We show that one can obtain asymptotic evolving boost-invariant geometries in
a simple manner from the corresponding static solutions. We exhibit the
procedure in the case of a supergravity dual of R-charged hydrodynamics by
turning on a supergravity gauge field and analyze the relevant thermodynamics.
Finally we con... | [
{
"created": "Tue, 28 Nov 2006 13:25:23 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Bak",
"Dongsu",
""
],
[
"Janik",
"Romuald A.",
""
]
] | We show that one can obtain asymptotic evolving boost-invariant geometries in a simple manner from the corresponding static solutions. We exhibit the procedure in the case of a supergravity dual of R-charged hydrodynamics by turning on a supergravity gauge field and analyze the relevant thermodynamics. Finally we consi... | 21.483446 | 18.274282 | 22.017418 | 19.558281 | 19.190733 | 20.926088 | 25.298222 | 19.45015 | 16.874664 | 22.490236 | 20.279436 | 20.181166 | 19.760548 | 19.312729 | 19.606606 | 18.250122 | 18.7869 | 19.724632 | 18.611931 | 20.822107 | 18.339424 |
2105.12594 | Junkai Dong | Junkai Dong, Thomas Hartman, and Yikun Jiang | Averaging over moduli in deformed WZW models | 22+17 pages | null | 10.1007/JHEP09(2021)185 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | WZW models live on a moduli space parameterized by current-current
deformations. The moduli space defines an ensemble of conformal field theories,
which generically have $N$ abelian conserved currents and central charge $c >
N$. We calculate the average partition function and show that it can be
interpreted as a sum ... | [
{
"created": "Wed, 26 May 2021 14:51:06 GMT",
"version": "v1"
},
{
"created": "Mon, 12 Jul 2021 21:42:41 GMT",
"version": "v2"
}
] | 2021-09-30 | [
[
"Dong",
"Junkai",
""
],
[
"Hartman",
"Thomas",
""
],
[
"Jiang",
"Yikun",
""
]
] | WZW models live on a moduli space parameterized by current-current deformations. The moduli space defines an ensemble of conformal field theories, which generically have $N$ abelian conserved currents and central charge $c > N$. We calculate the average partition function and show that it can be interpreted as a sum ov... | 9.108542 | 7.557524 | 10.669015 | 7.711402 | 8.169255 | 7.653202 | 8.346065 | 8.173413 | 7.808655 | 10.869841 | 7.987536 | 7.931618 | 8.930158 | 8.068786 | 8.070376 | 8.0869 | 7.962371 | 8.141003 | 8.252742 | 9.062782 | 8.263669 |
hep-th/0503005 | Jen-Chi Lee | Jen-Chi Lee | Generalized On-Shell Ward Identities in String Theory | null | Prog.Theor.Phys. 91 (1994) 353-360 | 10.1143/ptp/91.2.353 | null | hep-th | null | It is demonstrated that an infinite set of string-tree level on-shell Ward
identities, which are valid to all sigma-model loop orders, can be
systematically constructed without referring to the string field theory. As
examples, bosonic massive scattering amplitudes are calculated explicitly up to
the second massive e... | [
{
"created": "Tue, 1 Mar 2005 09:05:05 GMT",
"version": "v1"
}
] | 2017-02-01 | [
[
"Lee",
"Jen-Chi",
""
]
] | It is demonstrated that an infinite set of string-tree level on-shell Ward identities, which are valid to all sigma-model loop orders, can be systematically constructed without referring to the string field theory. As examples, bosonic massive scattering amplitudes are calculated explicitly up to the second massive exc... | 18.488691 | 17.432507 | 19.426661 | 16.655668 | 17.017397 | 17.970825 | 18.209509 | 16.635447 | 16.607454 | 21.817501 | 17.096926 | 16.372374 | 16.203407 | 16.348682 | 16.13904 | 16.538223 | 15.763218 | 16.403732 | 16.273108 | 18.035496 | 15.379917 |
hep-th/0105005 | Nicola Maggiore | N.Maggiore (Genoa U.) and A.Tanzini (LPTHE, Paris VI-VII) | Protected Operators in N=2,4 Supersymmetric Theories | 17 pages, no figures; some misprints corrected, references added | Nucl.Phys. B613 (2001) 34-48 | 10.1016/S0550-3213(01)00398-4 | GEF-TH-7/2001, LPTHE/01-22 | hep-th | null | The anomalous dimension of single and multi-trace composite operators of
scalar fields is shown to vanish at all orders of the perturbative series. The
proof hold for theories with N=2 supersymmetry with any number of
hypermultiplets in a generic representation of the gauge group. It then applies
to the finite N=4 th... | [
{
"created": "Tue, 1 May 2001 08:58:46 GMT",
"version": "v1"
},
{
"created": "Mon, 14 May 2001 13:49:24 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Maggiore",
"N.",
"",
"Genoa U."
],
[
"Tanzini",
"A.",
"",
"LPTHE, Paris VI-VII"
]
] | The anomalous dimension of single and multi-trace composite operators of scalar fields is shown to vanish at all orders of the perturbative series. The proof hold for theories with N=2 supersymmetry with any number of hypermultiplets in a generic representation of the gauge group. It then applies to the finite N=4 theo... | 8.787021 | 6.688059 | 9.360648 | 8.200641 | 8.110014 | 7.818098 | 7.34864 | 7.420329 | 7.54347 | 11.151129 | 7.234836 | 7.129154 | 8.184212 | 7.791845 | 7.911106 | 7.38166 | 7.225919 | 7.420633 | 7.321657 | 8.715044 | 7.649471 |
1805.07934 | Stam Nicolis | Stam Nicolis | Higher time derivatives in the microcanonical ensemble describe dynamics
of flux-coupled classical and quantum oscillators | 12 pages LaTeX2e | null | null | null | hep-th cond-mat.mes-hall gr-qc math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show that it is possible to consistently describe dynamical systems, whose
equations of motion are of degree higher than two, in the microcanonical
ensemble, even if the higher derivatives aren't coordinate artifacts. Higher
time derivatives imply that there are more than one Hamiltonians, conserved
quantities due... | [
{
"created": "Mon, 21 May 2018 08:05:01 GMT",
"version": "v1"
}
] | 2018-05-22 | [
[
"Nicolis",
"Stam",
""
]
] | We show that it is possible to consistently describe dynamical systems, whose equations of motion are of degree higher than two, in the microcanonical ensemble, even if the higher derivatives aren't coordinate artifacts. Higher time derivatives imply that there are more than one Hamiltonians, conserved quantities due t... | 13.746914 | 14.358245 | 14.375888 | 12.854351 | 13.452372 | 14.274918 | 14.286253 | 13.257058 | 13.030406 | 14.51817 | 13.270812 | 12.590812 | 13.012573 | 12.79061 | 12.623202 | 13.020425 | 12.465222 | 13.093465 | 12.867011 | 13.265491 | 12.972168 |
1712.07986 | Jeffrey Harvey | Jeffrey A. Harvey and Gregory W. Moore | Conway Subgroup Symmetric Compactifications Of Heterotic String | 42 pages | null | 10.1088/1751-8121/aac9d1 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate special compactifications of the heterotic string for which
the space of half-BPS states is, in a natural way, a representation of various
subgroups of the Conway group. These compactifications provide a useful
framework for analyzing the action of some of the large symmetry groups
appearing in discuss... | [
{
"created": "Thu, 21 Dec 2017 14:55:34 GMT",
"version": "v1"
}
] | 2018-08-15 | [
[
"Harvey",
"Jeffrey A.",
""
],
[
"Moore",
"Gregory W.",
""
]
] | We investigate special compactifications of the heterotic string for which the space of half-BPS states is, in a natural way, a representation of various subgroups of the Conway group. These compactifications provide a useful framework for analyzing the action of some of the large symmetry groups appearing in discussio... | 9.680444 | 8.839967 | 9.838533 | 8.088838 | 8.792362 | 9.27243 | 8.814799 | 8.166569 | 8.422824 | 11.089695 | 7.972589 | 8.88355 | 9.493889 | 8.663692 | 8.569162 | 8.725634 | 8.634951 | 8.888675 | 9.050284 | 9.383035 | 8.704245 |
hep-th/9310018 | Lars Brink | Lars Brink and Mikhail A. Vasiliev | Representations of the $S_N$-Extended Heisenberg Algebra and Relations
Between Knizhnik-Zamolodchikov Equations and Quantum Calogero Model | 7 pages | Mod.Phys.Lett. A8 (1993) 3585-3592 | 10.1142/S0217732393002324 | G\"{o}teborg ITP 93-42, FIAN/TD/18--93 | hep-th nlin.SI solv-int | null | We discuss lowest-weight representations of the $S_N$-Extended Heisenberg
Algebras underlying the $N$-body quantum-mechanical Calogero model. Our
construction leads to flat derivatives interpolating between
Knizhnik-Zamolodchikov and Dunkl derivatives. It is argued that based on these
results one can establish new li... | [
{
"created": "Mon, 4 Oct 1993 15:30:43 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Brink",
"Lars",
""
],
[
"Vasiliev",
"Mikhail A.",
""
]
] | We discuss lowest-weight representations of the $S_N$-Extended Heisenberg Algebras underlying the $N$-body quantum-mechanical Calogero model. Our construction leads to flat derivatives interpolating between Knizhnik-Zamolodchikov and Dunkl derivatives. It is argued that based on these results one can establish new link... | 9.208387 | 6.811116 | 10.289286 | 7.550961 | 8.604157 | 7.817133 | 7.829969 | 6.94073 | 7.306201 | 10.848691 | 7.272203 | 7.957456 | 8.724547 | 8.185219 | 8.124676 | 8.229037 | 7.859241 | 8.159276 | 7.877367 | 8.139718 | 7.884084 |
hep-th/9709168 | Andrei Mironov | A.Zabrodin | Zero curvature representation for classical lattice sine-Gordon equation
via quantum R-matrix | 10 pages, LaTeX (misprints are corrected) | JETP Lett. 66 (1997) 653-659 | 10.1134/1.567561 | ITEP-TH-47/97 | hep-th | null | Local M-operators for the classical sine-Gordon model in discrete space-time
are constructed by convolution of the quantum trigonometric 4$\times$4 R-matrix
with certain vectors in its "quantum" space. Components of the vectors are
identified with $\tau$-functions of the model. This construction generalizes
the known... | [
{
"created": "Tue, 23 Sep 1997 18:10:52 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Oct 1997 16:14:27 GMT",
"version": "v2"
}
] | 2009-10-30 | [
[
"Zabrodin",
"A.",
""
]
] | Local M-operators for the classical sine-Gordon model in discrete space-time are constructed by convolution of the quantum trigonometric 4$\times$4 R-matrix with certain vectors in its "quantum" space. Components of the vectors are identified with $\tau$-functions of the model. This construction generalizes the known r... | 13.76427 | 11.397287 | 15.713929 | 11.427691 | 12.316136 | 12.766293 | 13.188966 | 10.328677 | 12.048274 | 16.482307 | 10.972898 | 12.181478 | 12.648813 | 11.329024 | 11.5043 | 12.046365 | 12.35544 | 11.568643 | 11.524396 | 13.757944 | 11.768359 |
0912.5087 | Andjelo Samsarov | S.Meljanac, D.Meljanac, A.Samsarov, M.Stojic | Kappa-deformed Snyder spacetime | 12 pages, no figures, LaTeX2e class file, accepted for publication in
Modern Physics Letters A | Mod.Phys.Lett.A25:579-590,2010 | 10.1142/S0217732310032652 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present Lie-algebraic deformations of Minkowski space with undeformed
Poincare algebra. These deformations interpolate between Snyder and
kappa-Minkowski space. We find realizations of noncommutative coordinates in
terms of commutative coordinates and derivatives. Deformed Leibniz rule, the
coproduct structure and... | [
{
"created": "Sun, 27 Dec 2009 16:28:45 GMT",
"version": "v1"
}
] | 2010-04-30 | [
[
"Meljanac",
"S.",
""
],
[
"Meljanac",
"D.",
""
],
[
"Samsarov",
"A.",
""
],
[
"Stojic",
"M.",
""
]
] | We present Lie-algebraic deformations of Minkowski space with undeformed Poincare algebra. These deformations interpolate between Snyder and kappa-Minkowski space. We find realizations of noncommutative coordinates in terms of commutative coordinates and derivatives. Deformed Leibniz rule, the coproduct structure and s... | 9.054672 | 9.306267 | 9.391996 | 7.757761 | 8.351057 | 8.803406 | 9.172765 | 8.997921 | 8.954157 | 9.778102 | 8.475953 | 8.319954 | 9.292765 | 8.76912 | 8.694791 | 8.54948 | 8.48455 | 8.515522 | 8.830656 | 9.362534 | 8.507656 |
1107.2135 | David Ridout | Thomas Creutzig and David Ridout | Relating the Archetypes of Logarithmic Conformal Field Theory | 37 pages, 2 figures, several diagrams; v2 added a few paragraphs and
references | null | null | null | hep-th math-ph math.MP math.QA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Logarithmic conformal field theory is a rich and vibrant area of modern
mathematical physics with well-known applications to both condensed matter
theory and string theory. Our limited understanding of these theories is based
upon detailed studies of various examples that one may regard as archetypal.
These include t... | [
{
"created": "Mon, 11 Jul 2011 20:29:53 GMT",
"version": "v1"
},
{
"created": "Sat, 6 Apr 2013 01:14:43 GMT",
"version": "v2"
}
] | 2013-04-09 | [
[
"Creutzig",
"Thomas",
""
],
[
"Ridout",
"David",
""
]
] | Logarithmic conformal field theory is a rich and vibrant area of modern mathematical physics with well-known applications to both condensed matter theory and string theory. Our limited understanding of these theories is based upon detailed studies of various examples that one may regard as archetypal. These include the... | 6.924779 | 7.460956 | 9.785244 | 7.06506 | 7.413666 | 6.984315 | 7.493015 | 7.375657 | 6.78235 | 8.910508 | 7.027937 | 6.732435 | 8.061892 | 6.82243 | 6.748862 | 6.96209 | 6.841932 | 6.533835 | 6.751678 | 7.831709 | 6.834015 |
1706.07439 | Ritam Sinha | Adwait Gaikwad and Ritam Sinha | Spectral Form Factor in Non-Gaussian Random Matrix Theories | Introduction modified, section 2 moved to the Appendix, main text
slightly modified, section on Paley-Wiener theorem omitted, new perspective
on the results provided in sec V, typos corrected, footnotes added,
references added, conclusion unchanged | Phys. Rev. D 100, 026017 (2019) | 10.1103/PhysRevD.100.026017 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider Random Matrix Theories with non-Gaussian potentials that have a
rich phase structure in the large $N$ limit. We calculate the Spectral Form
Factor (SFF) in such models and present them as interesting examples of
dynamical models that display multi-criticality at short time-scales and
universality at large... | [
{
"created": "Thu, 22 Jun 2017 18:00:30 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Apr 2018 15:50:17 GMT",
"version": "v2"
},
{
"created": "Wed, 22 May 2019 13:18:53 GMT",
"version": "v3"
}
] | 2019-07-31 | [
[
"Gaikwad",
"Adwait",
""
],
[
"Sinha",
"Ritam",
""
]
] | We consider Random Matrix Theories with non-Gaussian potentials that have a rich phase structure in the large $N$ limit. We calculate the Spectral Form Factor (SFF) in such models and present them as interesting examples of dynamical models that display multi-criticality at short time-scales and universality at large t... | 10.839019 | 10.765488 | 12.325536 | 10.51457 | 10.68418 | 10.485104 | 10.686672 | 11.170415 | 9.981941 | 12.377637 | 10.362245 | 9.843939 | 10.699983 | 10.160589 | 10.054127 | 10.069929 | 10.033194 | 10.104948 | 9.893233 | 10.543118 | 9.714632 |
hep-th/0110002 | Emil | Emil T.Akhmedov (ITEP,Moscow) | Non-Abelian Structures in BSFT and RR couplings | Latex, 13pp., Minor correction (references added); This is the
extended version of the talk presented at 10th Tohwa International Symposium
on String theory which was held in Fukuoka, July 2001 | null | 10.1063/1.1454352 | ITEP-TH-53/01 | hep-th | null | In this talk we show that the tachyon annihilation combined with an
approximation, in which string theory non-commutativity structure is captured
by the algebra of differential operators on space-time, gives a unified point
of view on: non-Abelian structures on $D$-branes; all lowest energy excitations
on $D$-branes;... | [
{
"created": "Sat, 29 Sep 2001 13:55:59 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Oct 2001 11:46:48 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Akhmedov",
"Emil T.",
"",
"ITEP,Moscow"
]
] | In this talk we show that the tachyon annihilation combined with an approximation, in which string theory non-commutativity structure is captured by the algebra of differential operators on space-time, gives a unified point of view on: non-Abelian structures on $D$-branes; all lowest energy excitations on $D$-branes; a... | 15.813282 | 14.269009 | 17.68832 | 12.964049 | 13.059006 | 14.583658 | 12.78158 | 13.220527 | 13.376421 | 19.430603 | 14.089003 | 12.873142 | 16.839216 | 12.982001 | 12.977266 | 12.769037 | 12.871887 | 13.115167 | 13.025073 | 15.765341 | 12.692798 |
1305.5809 | Massimo Taronna | Euihun Joung, Massimo Taronna, Andrew Waldron | A Calculus for Higher Spin Interactions | 24 pages, 3 figures, LaTex. References added, typos corrected. Final
version to appear in JHEP | null | 10.1007/JHEP07(2013)186 | AEI-2013-211 | hep-th gr-qc math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Higher spin theories can be efficiently described in terms of auxiliary
St\"uckelberg or projective space field multiplets. By considering how higher
spin models couple to scale, these approaches can be unified in a conformal
geometry/tractor calculus framework. We review these methods and apply them to
higher spin v... | [
{
"created": "Fri, 24 May 2013 17:41:50 GMT",
"version": "v1"
},
{
"created": "Wed, 31 Jul 2013 18:39:58 GMT",
"version": "v2"
}
] | 2013-08-01 | [
[
"Joung",
"Euihun",
""
],
[
"Taronna",
"Massimo",
""
],
[
"Waldron",
"Andrew",
""
]
] | Higher spin theories can be efficiently described in terms of auxiliary St\"uckelberg or projective space field multiplets. By considering how higher spin models couple to scale, these approaches can be unified in a conformal geometry/tractor calculus framework. We review these methods and apply them to higher spin ver... | 23.523592 | 19.289383 | 21.783798 | 21.49869 | 21.832497 | 22.134398 | 22.96756 | 21.586472 | 20.494423 | 25.28389 | 19.721849 | 19.926722 | 22.309767 | 20.832291 | 21.441584 | 21.20755 | 21.129566 | 20.389812 | 21.741526 | 21.9401 | 21.357639 |
1905.03665 | Leonardo Giuliano Trombetta | Diana L\'opez Nacir, Francisco D. Mazzitelli, Leonardo G. Trombetta | To the sphere and back again: de Sitter infrared correlators at NTLO in
1/N | 10 pages, 1 figure | JHEP 08 (2019) 052 | 10.1007/JHEP08(2019)052 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the infrared behavior of the two and four-point functions for the
massless $O(N)$ model in Lorentzian de Sitter spacetime, using the $1/N$
expansion. Our approach is based in the study of the Schwinger-Dyson equations
on the sphere (Euclidean de Sitter space), using the fact that the infrared
behavior in L... | [
{
"created": "Thu, 9 May 2019 14:39:52 GMT",
"version": "v1"
},
{
"created": "Fri, 9 Aug 2019 09:31:58 GMT",
"version": "v2"
}
] | 2019-08-12 | [
[
"Nacir",
"Diana López",
""
],
[
"Mazzitelli",
"Francisco D.",
""
],
[
"Trombetta",
"Leonardo G.",
""
]
] | We analyze the infrared behavior of the two and four-point functions for the massless $O(N)$ model in Lorentzian de Sitter spacetime, using the $1/N$ expansion. Our approach is based in the study of the Schwinger-Dyson equations on the sphere (Euclidean de Sitter space), using the fact that the infrared behavior in Lor... | 6.38078 | 5.958598 | 6.667665 | 6.172649 | 6.150727 | 6.09402 | 5.943595 | 6.337376 | 6.249641 | 6.460044 | 6.009641 | 6.178055 | 6.359766 | 6.037127 | 6.266745 | 6.24541 | 6.135957 | 6.097818 | 6.095403 | 6.181652 | 5.953687 |
hep-th/0611264 | Bertrand Berche | Oleksandr Kapikranian (ICMP, LPM), Bertrand Berche (LPM), Yurij
Holovatch (ICMP) | Quasi-long-range ordering in a finite-size 2D Heisenberg model | 9 pages, 3 postscript figs, style files included | J.Phys.A40:3741-4748,2007 | 10.1088/1751-8113/40/14/001 | null | hep-th cond-mat.stat-mech hep-lat | null | We analyse the low-temperature behaviour of the Heisenberg model on a
two-dimensional lattice of finite size. Presence of a residual magnetisation in
a finite-size system enables us to use the spin wave approximation, which is
known to give reliable results for the XY model at low temperatures T. For the
system consi... | [
{
"created": "Fri, 24 Nov 2006 10:59:40 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Kapikranian",
"Oleksandr",
"",
"ICMP, LPM"
],
[
"Berche",
"Bertrand",
"",
"LPM"
],
[
"Holovatch",
"Yurij",
"",
"ICMP"
]
] | We analyse the low-temperature behaviour of the Heisenberg model on a two-dimensional lattice of finite size. Presence of a residual magnetisation in a finite-size system enables us to use the spin wave approximation, which is known to give reliable results for the XY model at low temperatures T. For the system conside... | 8.736627 | 9.565208 | 8.887024 | 8.690606 | 9.269011 | 9.624049 | 9.099036 | 8.927599 | 9.126792 | 8.684171 | 8.626783 | 8.710468 | 8.424047 | 8.606474 | 8.700371 | 8.726963 | 8.631826 | 8.654684 | 8.174054 | 8.535133 | 8.367445 |
1406.4147 | Florian Kuhnel | Florian Kuhnel, Bo Sundborg | High-Energy Gravitational Scattering and Bose-Einstein Condensates of
Gravitons | 8 pages, 1 figure | null | 10.1007/JHEP12(2014)016 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum black holes are difficult to describe. We consider two seemingly
divergent approaches, high-energy scattering and the proposal to regard black
holes as Bose-Einstein condensates of gravitons, and establish a connection
between them. High-energy scattering is studied in the eikonal approximation,
which is proc... | [
{
"created": "Mon, 16 Jun 2014 20:00:16 GMT",
"version": "v1"
}
] | 2015-06-22 | [
[
"Kuhnel",
"Florian",
""
],
[
"Sundborg",
"Bo",
""
]
] | Quantum black holes are difficult to describe. We consider two seemingly divergent approaches, high-energy scattering and the proposal to regard black holes as Bose-Einstein condensates of gravitons, and establish a connection between them. High-energy scattering is studied in the eikonal approximation, which is proces... | 9.401133 | 9.419488 | 9.65881 | 9.096874 | 10.092844 | 9.098151 | 9.294941 | 9.348569 | 9.023142 | 9.297651 | 9.066571 | 9.201656 | 9.296997 | 9.093744 | 9.226535 | 9.242862 | 9.153492 | 9.194121 | 9.218975 | 9.694332 | 9.24917 |
hep-th/0205029 | Stuart Dowker | J.S.Dowker and Klaus Kirsten | Elliptic functions and temperature inversion symmetry on spheres | 33 pages, JyTeX | Nucl.Phys. B638 (2002) 405-432 | 10.1016/S0550-3213(02)00477-7 | null | hep-th cond-mat | null | Finite temperature boson and fermion field theories on ultrastatic
space-times with a d-sphere spatial section are discussed with one eye on the
questions of temperature inversion symmetry and modular invariance. For
conformally invariant theories it is shown that the total energy at any
temperature for any dimension... | [
{
"created": "Fri, 3 May 2002 11:44:25 GMT",
"version": "v1"
}
] | 2015-06-26 | [
[
"Dowker",
"J. S.",
""
],
[
"Kirsten",
"Klaus",
""
]
] | Finite temperature boson and fermion field theories on ultrastatic space-times with a d-sphere spatial section are discussed with one eye on the questions of temperature inversion symmetry and modular invariance. For conformally invariant theories it is shown that the total energy at any temperature for any dimension, ... | 14.615462 | 12.98309 | 13.559936 | 12.921853 | 13.593166 | 12.923141 | 13.550733 | 12.310599 | 13.302401 | 16.449677 | 12.899014 | 13.460416 | 14.19171 | 13.599856 | 13.171632 | 12.62748 | 13.099789 | 13.306407 | 13.228454 | 13.949777 | 13.253959 |
0805.2610 | Daniel Grumiller | Daniel Grumiller and Niklas Johansson | Instability in cosmological topologically massive gravity at the chiral
point | 19 pages. v3: corrected sign mistake in (4.1) and related equations,
v4: corrected e-print number in Ref. [53] | JHEP 0807:134,2008 | 10.1088/1126-6708/2008/07/134 | MIT-CTP 3949, UUITP-08/08 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider cosmological topologically massive gravity at the chiral point
with positive sign of the Einstein-Hilbert term. We demonstrate the presence of
a negative energy bulk mode that grows linearly in time. Unless there are
physical reasons to discard this mode, this theory is unstable. To address this
issue we ... | [
{
"created": "Mon, 19 May 2008 18:18:42 GMT",
"version": "v1"
},
{
"created": "Thu, 29 May 2008 19:08:50 GMT",
"version": "v2"
},
{
"created": "Thu, 8 Oct 2009 16:31:19 GMT",
"version": "v3"
},
{
"created": "Thu, 22 Oct 2009 06:55:10 GMT",
"version": "v4"
}
] | 2010-05-12 | [
[
"Grumiller",
"Daniel",
""
],
[
"Johansson",
"Niklas",
""
]
] | We consider cosmological topologically massive gravity at the chiral point with positive sign of the Einstein-Hilbert term. We demonstrate the presence of a negative energy bulk mode that grows linearly in time. Unless there are physical reasons to discard this mode, this theory is unstable. To address this issue we pr... | 9.517327 | 10.161481 | 11.267239 | 9.44873 | 9.346289 | 10.378014 | 9.303612 | 9.406767 | 9.16392 | 11.349065 | 9.315798 | 9.490113 | 9.527693 | 9.581963 | 9.670121 | 9.637897 | 9.46296 | 9.431753 | 9.67414 | 9.851649 | 9.563713 |
1412.6373 | James Stevenson | Clare Burrage, Edmund J. Copeland, James Stevenson | Ellipticity Weakens Chameleon Screening | null | null | 10.1103/PhysRevD.91.065030 | null | hep-th astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The chameleon mechanism enables a long range fifth force to be screened in
dense environments when non-trivial self interactions of the field cause its
mass to increase with the local density. To date, chameleon fifth forces have
mainly been studied for spherically symmetric sources, however the non-linear
self inter... | [
{
"created": "Fri, 19 Dec 2014 15:21:22 GMT",
"version": "v1"
}
] | 2015-03-31 | [
[
"Burrage",
"Clare",
""
],
[
"Copeland",
"Edmund J.",
""
],
[
"Stevenson",
"James",
""
]
] | The chameleon mechanism enables a long range fifth force to be screened in dense environments when non-trivial self interactions of the field cause its mass to increase with the local density. To date, chameleon fifth forces have mainly been studied for spherically symmetric sources, however the non-linear self interac... | 9.836899 | 9.103198 | 7.927914 | 7.690631 | 7.799074 | 9.117715 | 8.543145 | 8.486633 | 7.871177 | 7.836937 | 8.020341 | 7.949946 | 7.305384 | 7.48109 | 7.966446 | 7.962042 | 7.659304 | 7.336069 | 7.331867 | 7.462193 | 7.609108 |
1702.00879 | Dionisio Bazeia | D. Bazeia, M.A. Marques, R. Menezes | Twinlike Models for Kinks, Vortices and Monopoles | 8 pages. New version, to appear in PRD | Phys. Rev. D 96, 025010 (2017) | 10.1103/PhysRevD.96.025010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work deals with twinlike models that support topological structures such
as kinks, vortices and monopoles. We investigate the equations of motion and
develop the first order framework to show how to build distinct models with the
same solution and energy density, as required to make them twinlike models. We
also... | [
{
"created": "Fri, 3 Feb 2017 00:34:59 GMT",
"version": "v1"
},
{
"created": "Wed, 21 Jun 2017 17:22:12 GMT",
"version": "v2"
}
] | 2017-07-19 | [
[
"Bazeia",
"D.",
""
],
[
"Marques",
"M. A.",
""
],
[
"Menezes",
"R.",
""
]
] | This work deals with twinlike models that support topological structures such as kinks, vortices and monopoles. We investigate the equations of motion and develop the first order framework to show how to build distinct models with the same solution and energy density, as required to make them twinlike models. We also i... | 12.591812 | 8.400004 | 11.969132 | 8.720028 | 8.597337 | 8.554989 | 8.105065 | 8.166849 | 8.539752 | 13.358783 | 9.607877 | 9.991793 | 12.005514 | 10.377222 | 10.272804 | 10.265642 | 9.884609 | 10.302843 | 10.368262 | 12.224466 | 10.589582 |
0705.1507 | Jae-Suk Park | Jae-Suk Park | Semi-Classical Quantum Fields Theories and Frobenius Manifolds | null | Lett.Math.Phys.81:41-59,2007 | 10.1007/s11005-007-0165-z | null | hep-th math.QA | null | We show that a semi-classical quantum field theory comes with a versal family
with the property that the corresponding partition function generates all path
integrals and satisfies a system of 2nd order differential equations determined
by algebras of classical observables. This versal family gives rise to a notion
o... | [
{
"created": "Thu, 10 May 2007 16:26:40 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Park",
"Jae-Suk",
""
]
] | We show that a semi-classical quantum field theory comes with a versal family with the property that the corresponding partition function generates all path integrals and satisfies a system of 2nd order differential equations determined by algebras of classical observables. This versal family gives rise to a notion of ... | 11.933833 | 12.026055 | 13.613372 | 11.743143 | 11.72486 | 12.65977 | 11.80167 | 11.486987 | 11.299418 | 14.621018 | 11.544922 | 11.378366 | 12.529982 | 11.457384 | 11.347363 | 11.802967 | 11.861361 | 11.652033 | 12.044722 | 12.242472 | 11.336263 |
2202.08056 | Dan Radu Grigore | Dan-Radu Grigore | Wick Theorem and Hopf Algebra Structure in Causal Perturbative Quantum
Field Theory | 57 pages, minor improvements. arXiv admin note: text overlap with
arXiv:2007.01115 | null | null | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | We consider the general framework of perturbative quantum field theory for
the pure Yang-Mills model. We give a more precise version of the Wick theorem
using Hopf algebra notations for chronological products and not for Feynman
graphs. Next we prove that Wick expansion property can be preserved for all
cases in orde... | [
{
"created": "Wed, 16 Feb 2022 13:40:47 GMT",
"version": "v1"
},
{
"created": "Thu, 11 Aug 2022 05:49:23 GMT",
"version": "v2"
}
] | 2022-08-12 | [
[
"Grigore",
"Dan-Radu",
""
]
] | We consider the general framework of perturbative quantum field theory for the pure Yang-Mills model. We give a more precise version of the Wick theorem using Hopf algebra notations for chronological products and not for Feynman graphs. Next we prove that Wick expansion property can be preserved for all cases in order ... | 20.788982 | 21.213215 | 22.854652 | 18.318645 | 19.382423 | 22.067337 | 19.628174 | 19.275 | 21.729643 | 25.167524 | 19.351805 | 19.426805 | 20.283915 | 18.775017 | 19.672623 | 20.527447 | 19.126232 | 18.980698 | 19.391987 | 19.011213 | 18.809549 |
1103.5468 | Daniel Grumiller | Mario Bertin, Daniel Grumiller, Dmitri Vassilevich and Thomas Zojer | Generalised massive gravity one-loop partition function and AdS/(L)CFT | 25 p., 2 jpg figs, v2: added 6 lines of clarifying text after Eq.
(2.38) | JHEP 1106:111,2011 | 10.1007/JHEP06(2011)111 | TUW-11-06 | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The graviton 1-loop partition function is calculated for Euclidean
generalised massive gravity (GMG) using AdS heat kernel techniques. We find
that the results fit perfectly into the AdS/(L)CFT picture. Conformal
Chern-Simons gravity, a singular limit of GMG, leads to an additional
contribution in the 1-loop determin... | [
{
"created": "Mon, 28 Mar 2011 20:03:24 GMT",
"version": "v1"
},
{
"created": "Wed, 8 Jun 2011 06:42:33 GMT",
"version": "v2"
}
] | 2011-06-28 | [
[
"Bertin",
"Mario",
""
],
[
"Grumiller",
"Daniel",
""
],
[
"Vassilevich",
"Dmitri",
""
],
[
"Zojer",
"Thomas",
""
]
] | The graviton 1-loop partition function is calculated for Euclidean generalised massive gravity (GMG) using AdS heat kernel techniques. We find that the results fit perfectly into the AdS/(L)CFT picture. Conformal Chern-Simons gravity, a singular limit of GMG, leads to an additional contribution in the 1-loop determinan... | 11.83602 | 10.416422 | 12.145857 | 10.494678 | 11.423548 | 9.54361 | 10.955988 | 10.531627 | 10.69872 | 12.534108 | 9.986703 | 10.330027 | 12.166821 | 10.739139 | 10.601548 | 10.429018 | 10.770862 | 10.772553 | 10.403282 | 11.318328 | 10.288692 |
1709.05057 | Michael M. Scherer | Nikolai Zerf, Luminita N. Mihaila, Peter Marquard, Igor F. Herbut,
Michael M. Scherer | Four-loop critical exponents for the Gross-Neveu-Yukawa models | 18 pages, 1 figure, 3 supplemental files attached containing the
critical exponents for general number of fermion flavors for each of the
models | Phys. Rev. D 96, 096010 (2017) | 10.1103/PhysRevD.96.096010 | null | hep-th cond-mat.str-el hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the chiral Ising, the chiral XY and the chiral Heisenberg models at
four-loop order with the perturbative renormalization group in $4-\epsilon$
dimensions and compute critical exponents for the Gross-Neveu-Yukawa fixed
points to order $\mathcal{O}(\epsilon^4)$. Further, we provide Pad\'e estimates
for the co... | [
{
"created": "Fri, 15 Sep 2017 04:45:34 GMT",
"version": "v1"
}
] | 2017-11-22 | [
[
"Zerf",
"Nikolai",
""
],
[
"Mihaila",
"Luminita N.",
""
],
[
"Marquard",
"Peter",
""
],
[
"Herbut",
"Igor F.",
""
],
[
"Scherer",
"Michael M.",
""
]
] | We study the chiral Ising, the chiral XY and the chiral Heisenberg models at four-loop order with the perturbative renormalization group in $4-\epsilon$ dimensions and compute critical exponents for the Gross-Neveu-Yukawa fixed points to order $\mathcal{O}(\epsilon^4)$. Further, we provide Pad\'e estimates for the corr... | 4.878128 | 5.728613 | 5.85968 | 5.381911 | 5.786466 | 5.473468 | 5.644255 | 5.512896 | 5.207759 | 6.439246 | 5.48611 | 5.140529 | 5.506166 | 5.189982 | 5.184308 | 5.274 | 5.188093 | 5.074058 | 5.120235 | 5.253855 | 5.18639 |
1207.6321 | Erik Panzer | Dirk Kreimer, Erik Panzer | Renormalization and Mellin transforms | 24 pages | Computer Algebra in Quantum Field Theory, Texts & Monographs in
Symbolic Computation, Springer Vienna, 2013, pp. 195-223 | 10.1007/978-3-7091-1616-6_8 | null | hep-th math-ph math.MP math.RA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study renormalization in a kinetic scheme using the Hopf algebraic
framework, first summarizing and recovering known results in this setting. Then
we give a direct combinatorial description of renormalized amplitudes in terms
of Mellin transform coefficients, featuring the universal property of rooted
trees H_R. I... | [
{
"created": "Thu, 26 Jul 2012 16:31:39 GMT",
"version": "v1"
}
] | 2014-01-20 | [
[
"Kreimer",
"Dirk",
""
],
[
"Panzer",
"Erik",
""
]
] | We study renormalization in a kinetic scheme using the Hopf algebraic framework, first summarizing and recovering known results in this setting. Then we give a direct combinatorial description of renormalized amplitudes in terms of Mellin transform coefficients, featuring the universal property of rooted trees H_R. In ... | 16.589174 | 17.436218 | 17.147591 | 16.885067 | 17.634859 | 17.006447 | 18.667513 | 17.09494 | 17.40406 | 18.420029 | 16.726734 | 16.624537 | 16.351757 | 16.004721 | 15.508249 | 16.319517 | 15.725504 | 15.818331 | 15.836758 | 16.248259 | 15.670676 |
0708.0439 | Changhyun Ahn | Changhyun Ahn | Meta-Stable Brane Configurations with Seven NS5-Branes | 34pp, 9 figures; Improved the draft and added some footnotes; Figure
1, footnote 7 and captions of Figures 7,8,9 added or improved and to appear
in CQG | Class.Quant.Grav.25:095018,2008 | 10.1088/0264-9381/25/9/095018 | KIAS-P07034 | hep-th | null | We present the intersecting brane configurations consisting of NS-branes,
D4-branes(and anti D4-branes) and O6-plane, of type IIA string theory
corresponding to the meta-stable nonsupersymmetric vacua in four dimensional
N=1 supersymmetric SU(N_c) x SU(N_c') x SU(N_c'') gauge theory with a symmetric
tensor field, a c... | [
{
"created": "Fri, 3 Aug 2007 00:04:00 GMT",
"version": "v1"
},
{
"created": "Mon, 3 Dec 2007 11:13:00 GMT",
"version": "v2"
},
{
"created": "Fri, 21 Mar 2008 04:12:48 GMT",
"version": "v3"
}
] | 2008-11-26 | [
[
"Ahn",
"Changhyun",
""
]
] | We present the intersecting brane configurations consisting of NS-branes, D4-branes(and anti D4-branes) and O6-plane, of type IIA string theory corresponding to the meta-stable nonsupersymmetric vacua in four dimensional N=1 supersymmetric SU(N_c) x SU(N_c') x SU(N_c'') gauge theory with a symmetric tensor field, a con... | 4.342332 | 3.360646 | 4.483238 | 3.452544 | 3.761285 | 3.465474 | 3.415941 | 3.35111 | 3.2458 | 4.550745 | 3.402311 | 3.839531 | 4.192316 | 3.976674 | 4.069104 | 3.779397 | 3.894022 | 3.983582 | 3.911953 | 4.286904 | 4.045857 |
0902.2453 | A. Tureanu | Masud Chaichian, Subir Ghosh, Miklos Langvik, Anca Tureanu | Dirac Quantization Condition for Monopole in Noncommutative Space-Time | 11 pages | Phys.Rev.D79:125029,2009 | 10.1103/PhysRevD.79.125029 | HIP-2009-02/TH | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Since the structure of space-time at very short distances is believed to get
modified possibly due to noncommutativity effects and as the Dirac Quantization
Condition (DQC), $\mu e = \frac{N}{2}\hbar c$, probes the magnetic field point
singularity, a natural question arises whether the same condition will still
survi... | [
{
"created": "Sat, 14 Feb 2009 10:55:15 GMT",
"version": "v1"
}
] | 2009-07-09 | [
[
"Chaichian",
"Masud",
""
],
[
"Ghosh",
"Subir",
""
],
[
"Langvik",
"Miklos",
""
],
[
"Tureanu",
"Anca",
""
]
] | Since the structure of space-time at very short distances is believed to get modified possibly due to noncommutativity effects and as the Dirac Quantization Condition (DQC), $\mu e = \frac{N}{2}\hbar c$, probes the magnetic field point singularity, a natural question arises whether the same condition will still survive... | 10.543964 | 11.404392 | 11.008221 | 10.249851 | 11.142075 | 11.027665 | 10.208707 | 10.347787 | 9.329389 | 10.335094 | 10.54254 | 9.745618 | 10.052547 | 9.712007 | 9.859972 | 9.78753 | 9.888046 | 9.934879 | 9.647429 | 10.023756 | 9.85634 |
hep-th/9605059 | Tomas Ortin Miguel | E. Bergshoeff, R. Kallosh, T. Ortin | Stationary Axion/Dilaton Solutions and Supersymmetry | A few comments added and alternative formulae for the horizon area
with manifest moduli-independence and duality-invariance given. 36 pages | Nucl.Phys.B478:156-180,1996 | 10.1016/0550-3213(96)00408-7 | UG-3/96, SU-ITP-19, CERN-TH/96-106 | hep-th | null | We present a new set of supersymmetric stationary solutions of pure N=4,d=4
supergravity (and, hence, of low-energy effective string theory) that
generalize (and include) the Israel-Wilson-Perj\'es solutions of
Einstein-Maxwell theory. All solutions have 1/4 of the supersymmetries unbroken
and some have 1/2. The full... | [
{
"created": "Wed, 8 May 1996 22:13:05 GMT",
"version": "v1"
},
{
"created": "Fri, 26 Jul 1996 09:54:16 GMT",
"version": "v2"
}
] | 2014-11-18 | [
[
"Bergshoeff",
"E.",
""
],
[
"Kallosh",
"R.",
""
],
[
"Ortin",
"T.",
""
]
] | We present a new set of supersymmetric stationary solutions of pure N=4,d=4 supergravity (and, hence, of low-energy effective string theory) that generalize (and include) the Israel-Wilson-Perj\'es solutions of Einstein-Maxwell theory. All solutions have 1/4 of the supersymmetries unbroken and some have 1/2. The full s... | 7.77578 | 7.707207 | 8.671951 | 7.090536 | 7.664564 | 8.15696 | 7.883866 | 7.684403 | 7.598874 | 8.615359 | 7.601255 | 7.301399 | 7.985906 | 7.676353 | 7.562159 | 7.626391 | 7.448408 | 7.683888 | 7.540997 | 8.014372 | 7.422475 |
2010.15838 | Thomas Grimm | Thomas W. Grimm | Moduli Space Holography and the Finiteness of Flux Vacua | 57 pages, 2 figures, v2: minor clarifications, typos corrected,
references added | JHEP 10 (2021) 153 | 10.1007/JHEP10(2021)153 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A holographic perspective to study and characterize field spaces that arise
in string compactifications is suggested. A concrete correspondence is
developed by studying two-dimensional moduli spaces in supersymmetric string
compactifications. It is proposed that there exist theories on the boundaries
of each moduli s... | [
{
"created": "Thu, 29 Oct 2020 18:00:00 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Mar 2021 16:03:08 GMT",
"version": "v2"
}
] | 2021-12-21 | [
[
"Grimm",
"Thomas W.",
""
]
] | A holographic perspective to study and characterize field spaces that arise in string compactifications is suggested. A concrete correspondence is developed by studying two-dimensional moduli spaces in supersymmetric string compactifications. It is proposed that there exist theories on the boundaries of each moduli spa... | 12.410127 | 12.657244 | 13.537525 | 11.248376 | 11.862572 | 11.93561 | 12.105978 | 11.428893 | 11.17994 | 13.913277 | 11.33514 | 11.967024 | 11.910478 | 11.627666 | 11.496089 | 11.406669 | 11.55993 | 11.513976 | 11.450241 | 12.128011 | 11.680659 |
1303.7120 | Sen Zhang | Sen Zhang | Pre-acceleration from Landau-Lifshitz Series | 16 pages | null | 10.1093/ptep/ptt099 | OIQP-13-05 | hep-th math-ph math.MP physics.class-ph physics.plasm-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Landau-Lifshitz equation is considered as an approximation of the
Abraham-Lorentz-Dirac equation. It is derived from the Abraham-Lorentz-Dirac
equation by treating radiation reaction terms as a perturbation. However, while
the Abraham-Lorentz-Dirac equation has pathological solutions of
pre-acceleration and runaw... | [
{
"created": "Thu, 28 Mar 2013 13:39:08 GMT",
"version": "v1"
}
] | 2014-05-07 | [
[
"Zhang",
"Sen",
""
]
] | The Landau-Lifshitz equation is considered as an approximation of the Abraham-Lorentz-Dirac equation. It is derived from the Abraham-Lorentz-Dirac equation by treating radiation reaction terms as a perturbation. However, while the Abraham-Lorentz-Dirac equation has pathological solutions of pre-acceleration and runaway... | 5.447296 | 5.984653 | 5.734529 | 5.607921 | 5.700387 | 6.11266 | 5.52748 | 6.096842 | 5.686289 | 5.857989 | 5.817919 | 5.550192 | 5.566045 | 5.338589 | 5.380095 | 5.440026 | 5.500269 | 5.455723 | 5.396396 | 5.56273 | 5.442892 |
hep-th/9907049 | Tatsuo Suzuki | Kazuyuki Fujii and Tatsuo Suzuki | A Universal Disentangling Formula for Coherent States of Perelomov's
Type | 11 pages, Latex2e | null | null | null | hep-th math-ph math.MP quant-ph | null | A universal disentangling formula (such as the Baker-Campbell-Hausdorff one)
for coherent states of Perelomov's type ($ |z \ra = \exp (z\Adag -\bar{z}A) |0
\ra $) which are defined for generalized oscillator algebras is given.
| [
{
"created": "Thu, 8 Jul 1999 06:28:40 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Fujii",
"Kazuyuki",
""
],
[
"Suzuki",
"Tatsuo",
""
]
] | A universal disentangling formula (such as the Baker-Campbell-Hausdorff one) for coherent states of Perelomov's type ($ |z \ra = \exp (z\Adag -\bar{z}A) |0 \ra $) which are defined for generalized oscillator algebras is given. | 11.112065 | 14.269137 | 13.295057 | 11.125383 | 12.503246 | 12.494489 | 14.174836 | 10.136027 | 13.180307 | 13.842218 | 11.690231 | 9.891302 | 11.557673 | 10.733949 | 9.894691 | 10.462368 | 9.880663 | 9.925301 | 10.264391 | 11.159222 | 10.555243 |
1304.6821 | Vladimir Rosenhaus | Stefan Leichenauer and Vladimir Rosenhaus | AdS black holes, the bulk-boundary dictionary, and smearing functions | 25 pages, published version | Phys. Rev. D 88, 026003 (2013) | 10.1103/PhysRevD.88.026003 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In Lorentzian AdS/CFT there exists a mapping between local bulk operators and
nonlocal CFT operators. In global AdS this mapping can be found through use of
bulk equations of motion and allows the nonlocal CFT operator to be expressed
as a local operator smeared over a range of positions and times. We argue that
such... | [
{
"created": "Thu, 25 Apr 2013 07:16:53 GMT",
"version": "v1"
},
{
"created": "Wed, 14 Aug 2013 07:15:04 GMT",
"version": "v2"
}
] | 2013-08-15 | [
[
"Leichenauer",
"Stefan",
""
],
[
"Rosenhaus",
"Vladimir",
""
]
] | In Lorentzian AdS/CFT there exists a mapping between local bulk operators and nonlocal CFT operators. In global AdS this mapping can be found through use of bulk equations of motion and allows the nonlocal CFT operator to be expressed as a local operator smeared over a range of positions and times. We argue that such a... | 9.641112 | 10.325209 | 10.253575 | 8.949893 | 10.574694 | 9.993465 | 10.084556 | 9.817098 | 9.995028 | 11.419287 | 9.674747 | 9.214405 | 9.682345 | 9.199041 | 9.235244 | 9.202334 | 9.158874 | 9.357059 | 9.079633 | 9.513094 | 9.253184 |
hep-th/0301032 | Angel M. Uranga | Angel M. Uranga | Chiral four-dimensional string compactifications with intersecting
D-branes | 30 pages, 16 figures, contribution to the proceedings of the TMR
meeting `The quantum structure of spacetime', Leuven, September 2002 | Class.Quant.Grav.20:S373-S394,2003 | 10.1088/0264-9381/20/12/303 | IFT-UAM-CSIC-02-03 | hep-th hep-ph | null | We review the construction of chiral four-dimensional compactifications of
type IIA string theory with intersecting D6-branes. Such models lead to
four-dimensional theories with non-abelian gauge interactions and charged
chiral fermions. We discuss the application of these techniques to building of
models with spectr... | [
{
"created": "Tue, 7 Jan 2003 12:01:21 GMT",
"version": "v1"
}
] | 2009-11-10 | [
[
"Uranga",
"Angel M.",
""
]
] | We review the construction of chiral four-dimensional compactifications of type IIA string theory with intersecting D6-branes. Such models lead to four-dimensional theories with non-abelian gauge interactions and charged chiral fermions. We discuss the application of these techniques to building of models with spectrum... | 8.932764 | 7.284 | 9.435941 | 7.53068 | 8.295263 | 8.376649 | 7.876436 | 7.368548 | 8.024673 | 10.375233 | 7.56005 | 8.052325 | 8.734964 | 7.983534 | 8.032491 | 7.976633 | 8.011336 | 8.039262 | 8.016063 | 8.578519 | 8.058196 |
0906.1177 | Fabio Riccioni | Fabio Riccioni, Duncan Steele and Peter West | The E(11) origin of all maximal supergravities - the hierarchy of
field-strengths | 87 pages, 8 figures. Typos corrected, refs added, other minor
changes. Version published on JHEP | JHEP 0909:095,2009 | 10.1088/1126-6708/2009/09/095 | KCL-MTH-09-05 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Starting from $E_{11}$ and the space-time translations we construct an
algebra that promotes the global $E_{11}$ symmetries to local ones, and
consider all its possible massive deformations. The Jacobi identities imply
that such deformations are uniquely determined by a single tensor that belongs
to the same represen... | [
{
"created": "Fri, 5 Jun 2009 18:29:23 GMT",
"version": "v1"
},
{
"created": "Thu, 1 Oct 2009 13:12:02 GMT",
"version": "v2"
}
] | 2009-10-02 | [
[
"Riccioni",
"Fabio",
""
],
[
"Steele",
"Duncan",
""
],
[
"West",
"Peter",
""
]
] | Starting from $E_{11}$ and the space-time translations we construct an algebra that promotes the global $E_{11}$ symmetries to local ones, and consider all its possible massive deformations. The Jacobi identities imply that such deformations are uniquely determined by a single tensor that belongs to the same representa... | 8.522795 | 7.447425 | 8.828389 | 7.470078 | 7.956868 | 8.070469 | 7.747334 | 7.467947 | 7.774629 | 9.240323 | 7.794876 | 7.584812 | 8.240655 | 7.657869 | 7.730656 | 7.891798 | 7.792865 | 7.507547 | 7.683269 | 8.007102 | 7.727464 |
hep-th/0604082 | Suguru Dobashi | Suguru Dobashi | Impurity Non-Preserving 3-Point Correlators of BMN Operators from
PP-Wave Holography II : Fermionic Excitations | 44 pages, 6 figures | Nucl.Phys.B756:171-206,2006 | 10.1016/j.nuclphysb.2006.08.004 | EPHOU-06-02 | hep-th | null | The holographic principle in the pp-wave limit proposed in our previous works
is further confirmed by studying impurity non-preserving processes which
contain a fermionic BMN operator with one scalar and one fermion impurities. We
show that the previously proposed duality relation between the matrix elements
of the t... | [
{
"created": "Tue, 11 Apr 2006 11:16:33 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Dobashi",
"Suguru",
""
]
] | The holographic principle in the pp-wave limit proposed in our previous works is further confirmed by studying impurity non-preserving processes which contain a fermionic BMN operator with one scalar and one fermion impurities. We show that the previously proposed duality relation between the matrix elements of the thr... | 11.532612 | 9.836237 | 11.87831 | 9.806437 | 10.155874 | 10.097499 | 10.015156 | 10.7814 | 10.245597 | 12.070592 | 9.877689 | 10.802282 | 11.507258 | 10.852173 | 10.967447 | 10.949561 | 10.617639 | 11.055053 | 10.806633 | 11.389182 | 10.990597 |
1709.07014 | Nemanja Kaloper | Guido D'Amico, Nemanja Kaloper, Albion Lawrence | Monodromy inflation at strong coupling: $4\pi$ in the sky | 11 pages LaTeX, 2 figures v2: a couple of small typos fixed | Phys. Rev. Lett. 121, 091301 (2018) | 10.1103/PhysRevLett.121.091301 | Brandeis preprint BRX-TH 6323, CERN preprint CERN-TH-2017-181 | hep-th astro-ph.CO gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a simple effective field theory formulation of a general family of
single field flux monodromy models for which strong coupling effects at large
field values can flatten the potential and activate operators with higher
powers of derivatives. These models are radiatively and non-perturbatively
stable and ca... | [
{
"created": "Wed, 20 Sep 2017 18:00:35 GMT",
"version": "v1"
},
{
"created": "Fri, 22 Sep 2017 15:39:50 GMT",
"version": "v2"
}
] | 2018-09-12 | [
[
"D'Amico",
"Guido",
""
],
[
"Kaloper",
"Nemanja",
""
],
[
"Lawrence",
"Albion",
""
]
] | We present a simple effective field theory formulation of a general family of single field flux monodromy models for which strong coupling effects at large field values can flatten the potential and activate operators with higher powers of derivatives. These models are radiatively and non-perturbatively stable and can ... | 11.339985 | 10.818277 | 12.170897 | 10.274114 | 11.906616 | 12.025413 | 11.73031 | 10.397017 | 10.288395 | 11.946433 | 10.366188 | 10.497285 | 11.026347 | 10.639929 | 10.644901 | 10.764582 | 10.533718 | 10.814899 | 10.731179 | 11.011775 | 10.909448 |
0808.3691 | Niclas Wyllard | Mirela Babalic, and Niclas Wyllard | Towards relating the kappa-symmetric and pure-spinor versions of the
supermembrane | 15 Pages | JHEP0810:059,2008 | 10.1088/1126-6708/2008/10/059 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the relation between the kappa-symmetric formulation of the
supermembrane in eleven dimensions and the pure-spinor version. Recently,
Berkovits related the Green-Schwarz and pure-spinor superstrings. In this
paper, we attempt to extend this method to the supermembrane. We show that it
is possible to reinstat... | [
{
"created": "Wed, 27 Aug 2008 12:54:09 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Babalic",
"Mirela",
""
],
[
"Wyllard",
"Niclas",
""
]
] | We study the relation between the kappa-symmetric formulation of the supermembrane in eleven dimensions and the pure-spinor version. Recently, Berkovits related the Green-Schwarz and pure-spinor superstrings. In this paper, we attempt to extend this method to the supermembrane. We show that it is possible to reinstate ... | 7.750425 | 7.693942 | 8.313724 | 7.174525 | 7.303112 | 7.805683 | 7.430104 | 7.070465 | 7.548618 | 9.312535 | 7.1566 | 7.342727 | 7.50285 | 7.128001 | 7.44468 | 7.279397 | 7.282948 | 7.451796 | 7.212488 | 7.724173 | 7.248416 |
1402.5674 | Leonard Susskind | Leonard Susskind | Computational Complexity and Black Hole Horizons | 44 pages, 18 figures | null | null | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Computational complexity is essential to understanding the properties of
black hole horizons. The problem of Alice creating a firewall behind the
horizon of Bob's black hole is a problem of computational complexity. In
general we find that while creating firewalls is possible, it is extremely
difficult and probably i... | [
{
"created": "Sun, 23 Feb 2014 21:01:02 GMT",
"version": "v1"
},
{
"created": "Tue, 25 Feb 2014 01:29:56 GMT",
"version": "v2"
}
] | 2014-02-26 | [
[
"Susskind",
"Leonard",
""
]
] | Computational complexity is essential to understanding the properties of black hole horizons. The problem of Alice creating a firewall behind the horizon of Bob's black hole is a problem of computational complexity. In general we find that while creating firewalls is possible, it is extremely difficult and probably imp... | 17.547136 | 18.80176 | 16.686754 | 16.890202 | 18.817339 | 17.848957 | 17.894585 | 19.797792 | 17.234798 | 20.183416 | 16.20484 | 16.64451 | 16.487999 | 17.031746 | 16.897112 | 17.681396 | 17.287529 | 16.964621 | 17.774366 | 16.221548 | 16.134481 |
hep-th/9701163 | Sergio Ferrara | Sergio Ferrara | Bertotti-Robinson Geometry and Supersymmetry | 13 pages, figures, uses procsla,epsf,epsfig; Talk given at the 12th
Italian Conference on General Relativity and Gravitational Physics, Rome,
September 1996 | null | null | CERN-TH/97-10 | hep-th | null | The role of Bertotti-Robinson geometry in the attractor mechanism of extremal
black holes is described for the case of N = 2 supersymmetry. Its implication
for a model-independent derivation of the Bekenstein-Hawking entropy formula is
discussed.
| [
{
"created": "Tue, 28 Jan 1997 16:40:44 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ferrara",
"Sergio",
""
]
] | The role of Bertotti-Robinson geometry in the attractor mechanism of extremal black holes is described for the case of N = 2 supersymmetry. Its implication for a model-independent derivation of the Bekenstein-Hawking entropy formula is discussed. | 8.805738 | 6.716015 | 7.364167 | 6.744504 | 6.54639 | 6.583862 | 6.127728 | 6.238834 | 6.753193 | 8.198648 | 7.090157 | 6.204502 | 6.847596 | 6.390301 | 6.245968 | 6.271868 | 6.151822 | 6.286191 | 6.452208 | 6.789905 | 7.028282 |
1801.03098 | Daniel Brattan K | Daniel K. Brattan | $\mathcal{N}=2$ supersymmetry and anisotropic scale invariance | 7 pages, 2 figures + 3 pages supplementary material; v2: minor typos
corrected and refs added | Phys. Rev. D 98, 036005 (2018) | 10.1103/PhysRevD.98.036005 | USTC-ICTS-18-03 | hep-th math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find a class of scale-anomaly-free $\mathcal{N}=2$ supersymmetric quantum
systems with non-vanishing potential terms where space and time scale with
distinct exponents. Our results generalise the known case of the supersymmetric
inverse square potential to a larger class of scaling symmetries.
| [
{
"created": "Tue, 9 Jan 2018 19:00:07 GMT",
"version": "v1"
},
{
"created": "Mon, 21 May 2018 12:50:19 GMT",
"version": "v2"
}
] | 2018-08-15 | [
[
"Brattan",
"Daniel K.",
""
]
] | We find a class of scale-anomaly-free $\mathcal{N}=2$ supersymmetric quantum systems with non-vanishing potential terms where space and time scale with distinct exponents. Our results generalise the known case of the supersymmetric inverse square potential to a larger class of scaling symmetries. | 14.112236 | 10.634133 | 12.784156 | 10.426134 | 10.367993 | 9.463438 | 10.683806 | 11.085165 | 10.576709 | 14.648897 | 10.254952 | 11.643295 | 11.919312 | 11.595649 | 11.173141 | 11.598697 | 10.801826 | 11.082709 | 11.705474 | 11.69063 | 10.886712 |
2307.02523 | Atsushi Ueda | Atsushi Ueda, Masahito Yamazaki | Fixed-point tensor is a four-point function | null | null | null | null | hep-th cond-mat.stat-mech cond-mat.str-el | http://creativecommons.org/licenses/by/4.0/ | Through coarse-graining, tensor network representations of a two-dimensional
critical lattice model flow to a universal four-leg tensor, corresponding to a
conformal field theory (CFT) fixed-point. We computed explicit elements of the
critical fixed-point tensor, which we identify as the CFT four-point function.
This... | [
{
"created": "Wed, 5 Jul 2023 18:00:00 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Aug 2023 05:32:30 GMT",
"version": "v2"
}
] | 2023-08-07 | [
[
"Ueda",
"Atsushi",
""
],
[
"Yamazaki",
"Masahito",
""
]
] | Through coarse-graining, tensor network representations of a two-dimensional critical lattice model flow to a universal four-leg tensor, corresponding to a conformal field theory (CFT) fixed-point. We computed explicit elements of the critical fixed-point tensor, which we identify as the CFT four-point function. This a... | 9.98595 | 12.802179 | 11.953397 | 10.010396 | 11.408174 | 11.601241 | 12.327858 | 10.433539 | 11.246507 | 13.535969 | 10.311706 | 10.076459 | 9.63248 | 9.987491 | 9.664013 | 9.895121 | 9.93011 | 10.136106 | 10.099438 | 10.478362 | 9.162732 |
hep-th/9402026 | Kazuhiro Hikami | Kazuhiro Hikami and Miki Wadati | On the Additional Symmetry; Many-Body Problem Related to the KP
Hierarchy | 8 pages | null | null | null | hep-th | null | Nonlinear integrable equations, such as the KdV equation, the Boussinesq
equation and the KP equation, have the close relation with many-body problem.
The solutions of such equations are the same as the restricted flows of the
classical Calogero model, which is one-dimensional particle system with inverse
square inte... | [
{
"created": "Fri, 4 Feb 1994 11:47:14 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Hikami",
"Kazuhiro",
""
],
[
"Wadati",
"Miki",
""
]
] | Nonlinear integrable equations, such as the KdV equation, the Boussinesq equation and the KP equation, have the close relation with many-body problem. The solutions of such equations are the same as the restricted flows of the classical Calogero model, which is one-dimensional particle system with inverse square intera... | 9.034881 | 8.398635 | 11.358582 | 8.853388 | 8.579323 | 8.992868 | 9.146437 | 9.069284 | 9.116944 | 11.196338 | 8.88189 | 8.382473 | 9.401574 | 8.335955 | 8.522663 | 8.213163 | 8.518147 | 8.449761 | 8.472001 | 9.433253 | 8.092966 |
hep-th/0306181 | Subir Ghosh | Subir Ghosh (Indian Statistical Institute) | The Seiberg-Witten Map in Noncommutative Field Theory: An Alternative
Interpretation | To appear in the special issue of the journal "Relativity,
Gravitation, Cosmology" | Rel.Grav.Cosmol. 1 (2004) 97-108 | null | null | hep-th | null | In this article, an alternative interpretation of the Seiberg-Witten map in
non-commutative field theory is provided. We show that the Seiberg-Witten map
can be induced in a geometric way, by a field dependent co-ordinate
transformation that connects noncommutative and ordinary space-times.
Furthermore, in continuati... | [
{
"created": "Thu, 19 Jun 2003 07:21:10 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Ghosh",
"Subir",
"",
"Indian Statistical Institute"
]
] | In this article, an alternative interpretation of the Seiberg-Witten map in non-commutative field theory is provided. We show that the Seiberg-Witten map can be induced in a geometric way, by a field dependent co-ordinate transformation that connects noncommutative and ordinary space-times. Furthermore, in continuation... | 9.700934 | 7.873993 | 9.272967 | 8.210982 | 9.150973 | 8.139362 | 8.523609 | 8.194945 | 8.162514 | 10.516006 | 7.842874 | 8.543727 | 8.824627 | 8.654179 | 8.611417 | 8.811692 | 8.395406 | 8.772663 | 8.884174 | 9.096953 | 8.741087 |
1010.4518 | Mairi Sakellariadou | Mairi Sakellariadou | Cosmological consequences of the noncommutative spectral geometry as an
approach to unification | 8 pages, Invited talk at the 14th Conference on recent Developments
in gravity (NEB 14), Ioannina, Greece, 8-11 June 2010 | J.Phys.Conf.Ser.283:012031,2011 | 10.1088/1742-6596/283/1/012031 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Noncommutative spectral geometry succeeds in explaining the physics of the
Standard Model of electroweak and strong interactions in all its details as
determined by experimental data. Moreover, by construction the theory lives at
very high energy scales, offering a natural framework to address early universe
cosmolog... | [
{
"created": "Thu, 21 Oct 2010 16:37:40 GMT",
"version": "v1"
}
] | 2011-03-21 | [
[
"Sakellariadou",
"Mairi",
""
]
] | Noncommutative spectral geometry succeeds in explaining the physics of the Standard Model of electroweak and strong interactions in all its details as determined by experimental data. Moreover, by construction the theory lives at very high energy scales, offering a natural framework to address early universe cosmologic... | 9.646518 | 8.021969 | 8.800497 | 8.521116 | 8.985275 | 8.421801 | 9.343526 | 7.822187 | 8.918799 | 9.002011 | 8.92016 | 9.453357 | 9.61397 | 8.944319 | 9.436932 | 8.649974 | 9.325676 | 8.776449 | 9.676103 | 9.066283 | 9.246678 |
0705.1233 | Peter Hess O | Peter O. Hess and Walter Greiner | Pseudo-Complex Field Theory | 21 pages, 1 figure | Int.J.Mod.Phys.E16:1643-1679,2007 | 10.1142/S0218301307006964 | null | hep-th | null | A new formulation of field theory is presented, based on a pseudo-complex
description. An extended group structure is introduced, implying a minimal
scalar length, rendering the theory regularized a la Pauli-Villars. Cross
sections are calculated for the scattering of an electron at an external
Coulomb field and the ... | [
{
"created": "Wed, 9 May 2007 09:00:43 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Hess",
"Peter O.",
""
],
[
"Greiner",
"Walter",
""
]
] | A new formulation of field theory is presented, based on a pseudo-complex description. An extended group structure is introduced, implying a minimal scalar length, rendering the theory regularized a la Pauli-Villars. Cross sections are calculated for the scattering of an electron at an external Coulomb field and the Co... | 13.056924 | 12.755198 | 12.91126 | 11.412694 | 13.378065 | 12.928124 | 12.825615 | 12.392459 | 13.001096 | 12.835352 | 12.839109 | 11.906312 | 11.903735 | 11.623879 | 11.392272 | 11.672449 | 11.633395 | 11.346335 | 12.331983 | 12.210276 | 11.875207 |
2208.04334 | Vasily Maslov | D. G. Levkov, V. E. Maslov, E. Ya. Nugaev, A. G. Panin | An Effective Field Theory for Large Oscillons | 43 pages, 9 figures, ancillary video of an oscillon formation; Sec. 5
and Appendix extended, references added; journal version | JHEP 12 (2022) 079 | 10.1007/JHEP12(2022)079 | INR-TH-2022-017 | hep-th astro-ph.CO hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider oscillons - localized, quasiperiodic, and extremely long-living
classical solutions in models with real scalar fields. We develop their
effective description in the limit of large size at finite field strength.
Namely, we note that nonlinear long-range field configurations can be described
by an effective... | [
{
"created": "Mon, 8 Aug 2022 18:00:03 GMT",
"version": "v1"
},
{
"created": "Tue, 29 Nov 2022 19:00:14 GMT",
"version": "v2"
}
] | 2022-12-19 | [
[
"Levkov",
"D. G.",
""
],
[
"Maslov",
"V. E.",
""
],
[
"Nugaev",
"E. Ya.",
""
],
[
"Panin",
"A. G.",
""
]
] | We consider oscillons - localized, quasiperiodic, and extremely long-living classical solutions in models with real scalar fields. We develop their effective description in the limit of large size at finite field strength. Namely, we note that nonlinear long-range field configurations can be described by an effective c... | 10.289037 | 11.817541 | 10.4505 | 10.260582 | 11.204687 | 11.081775 | 10.80305 | 10.14809 | 9.837203 | 11.649499 | 10.127261 | 10.322511 | 10.078436 | 10.115171 | 9.94995 | 10.286092 | 9.914851 | 10.273034 | 10.110717 | 10.280676 | 9.90336 |
1611.10290 | Seiji Terashima | Takahiro Nishinaka and Seiji Terashima | A Note on Sachdev-Ye-Kitaev Like Model without Random Coupling | 19 pages, 8 figures, references added | null | null | YITP-16-129 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study a description of the large N limit of the Sachdev-Ye-Kitaev (SYK)
model in terms of quantum mechanics without quenched disorder. Instead of
random couplings, we introduce massive scalar fields coupled to fermions, and
study a small mass limit of the theory. We show that, under a certain
condition, the correl... | [
{
"created": "Wed, 30 Nov 2016 17:52:14 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Nov 2017 09:12:41 GMT",
"version": "v2"
}
] | 2017-11-28 | [
[
"Nishinaka",
"Takahiro",
""
],
[
"Terashima",
"Seiji",
""
]
] | We study a description of the large N limit of the Sachdev-Ye-Kitaev (SYK) model in terms of quantum mechanics without quenched disorder. Instead of random couplings, we introduce massive scalar fields coupled to fermions, and study a small mass limit of the theory. We show that, under a certain condition, the correlat... | 5.58777 | 4.972653 | 6.151255 | 5.328371 | 5.100755 | 5.287951 | 5.066585 | 4.857635 | 5.112829 | 6.076184 | 5.274787 | 5.225568 | 5.748486 | 5.316951 | 5.255701 | 5.228495 | 5.175283 | 5.254071 | 5.247516 | 5.966405 | 5.270127 |
1807.10028 | Gaurav Narain | Gaurav Narain and Tianjun Li | Non-locality and late-time cosmic acceleration from an ultraviolet
complete theory | 1+9 pages. This manuscript belongs to an extension of the
International Conference on Quantum Gravity 2018, Shenzhen, China | Universe 2018, 4(8), 82 | 10.3390/universe4080082 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A local phenomenological model that reduces to a non-local gravitational
theory giving dark energy is proposed. The non-local gravity action is known to
fit the data as well as $\Lambda$-CDM thereby demanding a more fundamental
local treatment. It is seen that the scale-invariant higher-derivative
scalar-tensor theor... | [
{
"created": "Thu, 26 Jul 2018 09:25:16 GMT",
"version": "v1"
}
] | 2018-07-27 | [
[
"Narain",
"Gaurav",
""
],
[
"Li",
"Tianjun",
""
]
] | A local phenomenological model that reduces to a non-local gravitational theory giving dark energy is proposed. The non-local gravity action is known to fit the data as well as $\Lambda$-CDM thereby demanding a more fundamental local treatment. It is seen that the scale-invariant higher-derivative scalar-tensor theory ... | 11.960244 | 12.312081 | 12.812638 | 11.433576 | 12.373528 | 12.303228 | 12.193257 | 11.204792 | 11.265106 | 13.574794 | 11.476741 | 11.442659 | 11.961074 | 11.499356 | 11.494163 | 11.454371 | 11.46174 | 11.485919 | 11.453451 | 11.747772 | 11.062652 |
2210.06762 | Jun Nian | Jun Nian, Xiaoquan Yu, Jinwu Ye | A Non-Unitary Conformal Field Theory Approach to Two-Dimensional
Turbulence | 19+19 pages, 3 figures | null | null | null | hep-th cond-mat.stat-mech nlin.CD physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Fluid turbulence is a far-from-equilibrium phenomenon and remains one of the
most challenging problems in physics. Two-dimensional, fully developed
turbulence may possess the largest possible symmetry, the conformal symmetry.
We focus on the steady-state solution of two-dimensional bounded turbulent flow
and propose ... | [
{
"created": "Thu, 13 Oct 2022 06:07:43 GMT",
"version": "v1"
}
] | 2022-10-14 | [
[
"Nian",
"Jun",
""
],
[
"Yu",
"Xiaoquan",
""
],
[
"Ye",
"Jinwu",
""
]
] | Fluid turbulence is a far-from-equilibrium phenomenon and remains one of the most challenging problems in physics. Two-dimensional, fully developed turbulence may possess the largest possible symmetry, the conformal symmetry. We focus on the steady-state solution of two-dimensional bounded turbulent flow and propose a ... | 7.9489 | 8.965986 | 8.933343 | 7.673749 | 7.978081 | 8.452511 | 8.569606 | 8.698277 | 7.989566 | 9.373913 | 7.186038 | 7.784334 | 8.208424 | 7.726233 | 7.74149 | 7.898304 | 7.429446 | 7.809169 | 7.722451 | 8.217149 | 7.492542 |
hep-th/9904093 | Jose M. Carmona | J.M. Carmona, J. Polonyi and A. Tarancon | Wegner-Houghton equation in low dimensions | 44 pages, 9 figures; some sections revised, refs. added; final
version to appear in Phys. Rev. D | Phys.Rev. D61 (2000) 085018 | 10.1103/PhysRevD.61.085018 | IFUP-TH-18/99 | hep-th | null | We consider scalar field theories in dimensions lower than four in the
context of the Wegner-Houghton renormalization group equations (WHRG). The
renormalized trajectory makes a non-perturbative interpolation between the
ultraviolet and the infrared scaling regimes. Strong indication is found that
in two dimensions a... | [
{
"created": "Tue, 13 Apr 1999 16:51:06 GMT",
"version": "v1"
},
{
"created": "Tue, 18 Jan 2000 11:51:07 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Carmona",
"J. M.",
""
],
[
"Polonyi",
"J.",
""
],
[
"Tarancon",
"A.",
""
]
] | We consider scalar field theories in dimensions lower than four in the context of the Wegner-Houghton renormalization group equations (WHRG). The renormalized trajectory makes a non-perturbative interpolation between the ultraviolet and the infrared scaling regimes. Strong indication is found that in two dimensions and... | 9.727388 | 9.024496 | 10.675576 | 9.389061 | 9.813466 | 8.978375 | 9.529517 | 8.406079 | 8.831871 | 10.850271 | 9.105037 | 9.333596 | 10.22921 | 9.557647 | 9.279192 | 9.397818 | 9.440052 | 9.706614 | 9.104889 | 10.272797 | 9.357285 |
hep-th/0009192 | Silvia | S.J. Gates, Jr., M.T. Grisaru, M.E. Knutt, S. Penati, H. Suzuki | Supersymmetric Gauge Anomaly with General Homotopic Paths | 36 pages, plain Latex, no figures | Nucl.Phys. B596 (2001) 315-347 | 10.1016/S0550-3213(00)00676-3 | Bicocca-FT-00-13, BRX TH-479, IU-MSTP/41, McGill 00-28, UMDEPP
01-098 | hep-th | null | We use the method of Banerjee, Banerjee and Mitra and minimal homotopy paths
to compute the consistent gauge anomaly for several superspace models of SSYM
coupled to matter. We review the derivation of the anomaly for N=1 in four
dimensions and then discuss the anomaly for two-dimensional models with (2,0)
supersymme... | [
{
"created": "Mon, 25 Sep 2000 15:22:41 GMT",
"version": "v1"
}
] | 2012-08-27 | [
[
"Gates,",
"S. J.",
"Jr."
],
[
"Grisaru",
"M. T.",
""
],
[
"Knutt",
"M. E.",
""
],
[
"Penati",
"S.",
""
],
[
"Suzuki",
"H.",
""
]
] | We use the method of Banerjee, Banerjee and Mitra and minimal homotopy paths to compute the consistent gauge anomaly for several superspace models of SSYM coupled to matter. We review the derivation of the anomaly for N=1 in four dimensions and then discuss the anomaly for two-dimensional models with (2,0) supersymmetr... | 17.107298 | 14.532182 | 19.553017 | 14.208922 | 14.24106 | 16.523457 | 16.65336 | 14.67239 | 14.568316 | 19.176308 | 13.98838 | 14.040052 | 16.294233 | 14.057124 | 14.298664 | 14.79585 | 14.166024 | 14.412909 | 15.213874 | 16.462605 | 13.950874 |
hep-th/9504097 | Jan De Boer | Jan de Boer, Bas Peeters, Kostas Skenderis and Peter van Nieuwenhuizen | Loop calculations in quantum-mechanical non-linear sigma models | 17 pages, LaTeX, and one figure | Nucl.Phys. B446 (1995) 211-222 | 10.1016/0550-3213(95)00241-J | ITP-SB-95-12 | hep-th | null | By carefully analyzing the relations between operator methods and the
discretized and continuum path integral formulations of quantum-mechanical
systems, we have found the correct Feynman rules for one-dimensional path
integrals in curved spacetime. Although the prescription how to deal with the
products of distribut... | [
{
"created": "Wed, 19 Apr 1995 17:30:23 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"de Boer",
"Jan",
""
],
[
"Peeters",
"Bas",
""
],
[
"Skenderis",
"Kostas",
""
],
[
"van Nieuwenhuizen",
"Peter",
""
]
] | By carefully analyzing the relations between operator methods and the discretized and continuum path integral formulations of quantum-mechanical systems, we have found the correct Feynman rules for one-dimensional path integrals in curved spacetime. Although the prescription how to deal with the products of distributio... | 13.904754 | 11.101833 | 11.374455 | 11.436378 | 11.781695 | 11.522929 | 11.964627 | 10.999715 | 11.477244 | 12.535537 | 11.551274 | 11.460671 | 11.428762 | 11.044684 | 11.327518 | 11.024455 | 10.986031 | 11.476747 | 11.376809 | 11.788137 | 11.291865 |
0910.5202 | Brett D. Altschul | Alejandro Ferrero and Brett Altschul | Radiatively Induced Lorentz and Gauge Symmetry Violation in
Electrodynamics with Varying alpha | 14 pages | Phys.Rev.D80:125010,2009 | 10.1103/PhysRevD.80.125010 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A time-varying fine structure constant alpha(t) could give rise to Lorentz-
and CPT-violating changes to the vacuum polarization, which would affect photon
propagation. Such changes to the effective action can violate gauge invariance,
but they are otherwise permitted. However, in the minimal theory of varying
alpha,... | [
{
"created": "Tue, 27 Oct 2009 18:40:15 GMT",
"version": "v1"
}
] | 2009-12-30 | [
[
"Ferrero",
"Alejandro",
""
],
[
"Altschul",
"Brett",
""
]
] | A time-varying fine structure constant alpha(t) could give rise to Lorentz- and CPT-violating changes to the vacuum polarization, which would affect photon propagation. Such changes to the effective action can violate gauge invariance, but they are otherwise permitted. However, in the minimal theory of varying alpha, n... | 12.174788 | 12.186724 | 11.902003 | 10.337322 | 12.005235 | 11.315409 | 11.378343 | 10.798018 | 10.279054 | 11.955226 | 11.738037 | 10.89895 | 10.997777 | 10.782282 | 11.017561 | 11.422002 | 11.350824 | 10.765131 | 10.921099 | 11.075354 | 11.492403 |
1709.06323 | Arata Yamamoto | Arata Yamamoto | One-dimensional anyons in relativistic field theory | null | PTEP 2018 (2018) 043B03 | 10.1093/ptep/pty030 | null | hep-th cond-mat.stat-mech hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study relativistic anyon field theory in 1+1 dimensions. While
(2+1)-dimensional anyon fields are equivalent to boson or fermion fields
coupled with the Chern-Simons gauge fields, (1+1)-dimensional anyon fields are
equivalent to boson or fermion fields with many-body interaction. We derive the
path integral repres... | [
{
"created": "Tue, 19 Sep 2017 10:01:29 GMT",
"version": "v1"
},
{
"created": "Fri, 23 Feb 2018 11:50:39 GMT",
"version": "v2"
}
] | 2018-04-11 | [
[
"Yamamoto",
"Arata",
""
]
] | We study relativistic anyon field theory in 1+1 dimensions. While (2+1)-dimensional anyon fields are equivalent to boson or fermion fields coupled with the Chern-Simons gauge fields, (1+1)-dimensional anyon fields are equivalent to boson or fermion fields with many-body interaction. We derive the path integral represen... | 5.975152 | 5.691713 | 5.693698 | 5.176709 | 5.785944 | 5.534485 | 5.743881 | 5.056806 | 5.12703 | 6.114923 | 5.247338 | 5.521801 | 5.710806 | 5.577816 | 5.698193 | 5.744758 | 5.409414 | 5.513401 | 5.506699 | 5.536954 | 5.419868 |
0910.5596 | Stefan Hohenegger | I. Antoniadis and S. Hohenegger | N=4 Topological Amplitudes and Black Hole Entropy | 33 pages, references added, section 3.3 added | Nucl.Phys.B837:61-89,2010 | 10.1016/j.nuclphysb.2010.04.026 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the effects of N=4 topological string amplitudes on the entropy of
black holes. We analyse the leading contribution associated to six-derivative
terms and find one particular operator which can correct the entropy of N=4
black holes. This operator is BPS-like and appears in the effective action of
type II st... | [
{
"created": "Thu, 29 Oct 2009 09:46:41 GMT",
"version": "v1"
},
{
"created": "Sun, 2 May 2010 15:46:44 GMT",
"version": "v2"
}
] | 2014-11-20 | [
[
"Antoniadis",
"I.",
""
],
[
"Hohenegger",
"S.",
""
]
] | We study the effects of N=4 topological string amplitudes on the entropy of black holes. We analyse the leading contribution associated to six-derivative terms and find one particular operator which can correct the entropy of N=4 black holes. This operator is BPS-like and appears in the effective action of type II stri... | 11.326788 | 11.515522 | 12.00106 | 10.798276 | 11.124301 | 11.149722 | 11.218502 | 10.503621 | 10.514576 | 12.151256 | 10.810825 | 10.916337 | 10.924257 | 10.536064 | 10.900265 | 10.640753 | 10.986974 | 10.733359 | 10.669917 | 10.910553 | 10.57512 |
2003.04349 | Nabil Iqbal | Nabil Iqbal and John McGreevy | Toward a 3d Ising model with a weakly-coupled string theory dual | 34 pages + appendices. Many plots and pictures of cubes. Appendix E
can be cut out and assembled. Code available at
https://github.com/nabiliqbal/3d-ising-string-theory. v2: references added,
minor changes | SciPost Phys. 9, 019 (2020) | 10.21468/SciPostPhys.9.2.019 | null | hep-th cond-mat.stat-mech cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It has long been expected that the 3d Ising model can be thought of as a
string theory, where one interprets the domain walls that separate up spins
from down spins as two-dimensional string worldsheets. The usual Ising
Hamiltonian measures the area of these domain walls. This theory has string
coupling of unit magni... | [
{
"created": "Mon, 9 Mar 2020 18:31:29 GMT",
"version": "v1"
},
{
"created": "Tue, 16 Jun 2020 12:18:40 GMT",
"version": "v2"
}
] | 2020-08-19 | [
[
"Iqbal",
"Nabil",
""
],
[
"McGreevy",
"John",
""
]
] | It has long been expected that the 3d Ising model can be thought of as a string theory, where one interprets the domain walls that separate up spins from down spins as two-dimensional string worldsheets. The usual Ising Hamiltonian measures the area of these domain walls. This theory has string coupling of unit magnitu... | 8.689496 | 8.411841 | 9.005779 | 7.712826 | 8.189082 | 8.142051 | 8.474369 | 8.062003 | 8.286366 | 9.687749 | 8.050966 | 7.817602 | 8.358521 | 7.780116 | 7.200536 | 7.474385 | 7.537556 | 7.727673 | 7.82417 | 8.630382 | 7.639908 |
hep-th/0503214 | Akifumi Sako | Akifumi Sako, Toshiya Suzuki | Partition functions of Supersymmetric Gauge Theories in Noncommutative
R^{2D} and their Unified Perspective | 45 pages, no figures, Appendices B and C are added, changes in the
text, references are added | J.Math.Phys. 47 (2006) 012303 | 10.1063/1.2162127 | OCHA-PP-249, KSTS/RR-05/002 | hep-th math-ph math.MP | null | We investigate cohomological gauge theories in noncommutative R^{2D}. We show
that vacuum expectation values of the theories do not depend on noncommutative
parameters, and the large noncommutative parameter limit is equivalent to the
dimensional reduction. As a result of these facts, we show that a partition
functio... | [
{
"created": "Sun, 27 Mar 2005 16:44:12 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Apr 2005 19:21:52 GMT",
"version": "v2"
},
{
"created": "Sat, 30 Apr 2005 14:23:57 GMT",
"version": "v3"
},
{
"created": "Wed, 30 Nov 2005 05:17:01 GMT",
"version": "v4"
}
] | 2009-11-11 | [
[
"Sako",
"Akifumi",
""
],
[
"Suzuki",
"Toshiya",
""
]
] | We investigate cohomological gauge theories in noncommutative R^{2D}. We show that vacuum expectation values of the theories do not depend on noncommutative parameters, and the large noncommutative parameter limit is equivalent to the dimensional reduction. As a result of these facts, we show that a partition function ... | 6.341418 | 5.995378 | 6.56216 | 5.827777 | 6.220135 | 5.984005 | 6.062258 | 5.864358 | 5.965291 | 7.140497 | 5.816127 | 6.196927 | 6.459914 | 6.047641 | 6.031993 | 6.029497 | 6.109245 | 5.998647 | 6.188897 | 6.467417 | 5.980451 |
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