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hep-lat/9107001
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How to Put a Heavier Higgs on the Lattice
Lattice work, exploring the Higgs mass triviality bound, seems to indicate that a strongly interacting scalar sector in the minimal standard model cannot exist while low energy QCD phenomenology seems to indicate that it could. We attack this puzzle using the 1/N expansion and discover a simple criterion for selectin...
U.M. Heller, H. Neuberger and P. Vranas
hep-lat
July
1,991
https://arxiv.org/abs/hep-lat/9107001
hep-lat/9107002
[ 0.2925231158733368, 0.2564675509929657, 0.3746941387653351, 0.21110357344150543, 0.3264656364917755, -0.2669422924518585, -0.39229756593704224, -0.24725304543972015, -0.7059420347213745, 1.271836519241333, 0.6093198657035828, 0.12722910940647125, 0.32144710421562195, -1.0756332874298096, ...
Spectral Density Study of the SU(3) Deconfining Phase Transition
We present spectral density reweighting techniques adapted to the analysis of a time series of data with a continuous range of allowed values. In a first application we analyze action and Polyakov line data from a Monte Carlo simulation on $L_t L^3 (L_t=2,4)$ lattices for the SU(3) deconfining phase transition. We ca...
Nelsons A. Alves, Bernd Al. Berg and Sergiu Sanielevici
hep-lat
July
1,991
https://arxiv.org/abs/hep-lat/9107002
hep-lat/9112001
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Vectorized Cluster Search
Contrary to conventional wisdom, the construction of clusters on a lattice can easily be vectorized, namely over each ``generation'' in a breadth first search. This applies directly to, e.g., the {\it single cluster} variant of the Swendsen-Wang algorithm. On a Cray Y-MP, total CPU time was reduced by a factor 3.5 --...
Hans Gerd Evertz
hep-lat
December
1,991
https://arxiv.org/abs/hep-lat/9112001
hep-lat/9112002
[ 0.8349723815917969, 0.2653530240058899, -0.13327445089817047, 0.2925688326358795, -0.0031967945396900177, -0.3683493435382843, -0.05592067912220955, -0.5107839107513428, -0.2862716615200043, 1.2930835485458374, 0.7854194045066833, -0.14445051550865173, 0.16884705424308777, -1.3421412706375...
Multi-Grid Monte Carlo III. Two-Dimensional O(4)-Symmetric Nonlinear $\sigma$-Model
We study the dynamic critical behavior of the multi-grid Monte Carlo (MGMC) algorithm with piecewise-constant interpolation applied to the two-dimensional O(4)-symmetric nonlinear $\sigma$-model [= SU(2) principal chiral model], on lattices up to $256 \times 256$. We find a dynamic critical exponent $z_{int,{\cal M}^...
Robert G. Edwards, Sabino Jos\'e Ferreira, Jonathan Goodman, Alan D. Sokal
hep-lat
December
1,991
https://arxiv.org/abs/hep-lat/9112002
hep-th/9108001
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Exact Black String Solutions in Three Dimensions
A family of exact conformal field theories is constructed which describe charged black strings in three dimensions. Unlike previous charged black hole or extended black hole solutions in string theory, the low energy spacetime metric has a regular inner horizon (in addition to the event horizon) and a timelike singul...
James H. Horne and Gary T. Horowitz
hep-th
August
1,991
https://arxiv.org/abs/hep-th/9108001
hep-th/9108002
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Hamiltonian construction of W-gravity actions
We show that all W-gravity actions can be easilly constructed and understood from the point of view of the Hamiltonian formalism for the constrained systems. This formalism also gives a method of constructing gauge invariant actions for arbitrary conformally extended algebras.
A. Mikovic
hep-th
August
1,991
https://arxiv.org/abs/hep-th/9108002
hep-th/9108003
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Supersymmetric Gelfand-Dickey Algebra
We study the classical version of supersymmetric $W$-algebras. Using the second Gelfand-Dickey Hamiltonian structure we work out in detail $W_2$ and $W_3$-algebras.
Katri Huitu and Dennis Nemeschansky
hep-th
August
1,991
https://arxiv.org/abs/hep-th/9108003
hep-th/9108004
[ 0.5581084489822388, 0.29739242792129517, 0.39769819378852844, -0.35875850915908813, 0.5726051330566406, -0.7257758378982544, -0.3120996057987213, 0.17615534365177155, -0.5648409128189087, 1.902421474456787, 0.6871086359024048, 0.4191212058067322, 0.2734951674938202, -0.8752585053443909, ...
Ground Ring Of Two Dimensional String Theory
String theories with two dimensional space-time target spaces are characterized by the existence of a ``ground ring'' of operators of spin $(0,0)$. By understanding this ring, one can understand the symmetries of the theory and illuminate the relation of the critical string theory to matrix models. The symmetry group...
Edward Witten
hep-th
August
1,991
https://arxiv.org/abs/hep-th/9108004
hep-th/9108005
[ 0.2715948820114136, -0.14874158799648285, 0.2998250126838684, 0.783498227596283, 0.4887743592262268, -0.09863106906414032, 0.25902464985847473, -0.25786271691322327, -1.0808196067810059, 1.489359736442566, 0.613923192024231, 0.1489780992269516, -0.06728275120258331, -0.8631169199943542, ...
Fusion Residues
We discuss when and how the Verlinde dimensions of a rational conformal field theory can be expressed as correlation functions in a topological LG theory. It is seen that a necessary condition is that the RCFT fusion rules must exhibit an extra symmetry. We consider two particular perturbations of the Grassmannian su...
Kenneth Intriligator
hep-th
August
1,991
https://arxiv.org/abs/hep-th/9108005
hep-th/9108006
[-0.41452136635780334,-0.38981708884239197,-0.17891845107078552,-0.3902316093444824,0.51325500011444(...TRUNCATED)
Discrete and Continuum Approaches to Three-Dimensional Quantum Gravity
" It is shown that, in the three-dimensional lattice gravity defined by Ponzano and Regge, the spac(...TRUNCATED)
Hirosi Ooguri and Naoki Sasakura
hep-th
August
1,991
https://arxiv.org/abs/hep-th/9108006
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