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| [[image:Exact_diag.jpg|100px|center|frame|Exact diagonalization algorithm for Dynamical mean field theory (see [[Caffarel Krauth 1994|article with M. Caffarel]]). This algorithm has been instrumental in our discovery of a first-order Mott transition in the Hubbard model in infinite dimensions. Much of our early work in the field is written up in our [[Georges_Kotliar_Krauth_Rozenberg_1996|review with Georges, Kotliar, and Rozenberg]]]] | [[image:Exact_diag.jpg|100px|center|frame|Exact diagonalization algorithm for Dynamical mean field theory (see [[Caffarel Krauth 1994|article with M. Caffarel]]). This algorithm has been instrumental in our discovery of a first-order Mott transition in the Hubbard model in infinite dimensions. Much of our early work in the field is written up in our [[Georges_Kotliar_Krauth_Rozenberg_1996|review with Georges, Kotliar, and Rozenberg]]]] | ||
| - | [[image:Dimer_cluster.gif|100px|right|frame|Rejection-free cluster algorithm for dimers (see [[Krauth Moessner 2003|article with R. Moessner]]). This algorithm was used for our discovery of a critical phase in three-dimensional dimer models (paper with Huse, Sondhi, and Moessner). Note that dimers move with respect to a symmetry axis between two valid configurations.]] | + | [[image:Dimer_cluster.gif|100px|right|frame|Rejection-free cluster algorithm for dimers (see [[Krauth Moessner 2003|article with R. Moessner]]). This algorithm was used for our discovery of a critical phase in three-dimensional dimer models ([[Huse Krauth Moessner Sondhi 2003|paper with Huse, Sondhi, and Moessner]]). Note that dimers flip about a symmetry axis between one valid configuration and another.]] |
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Revision as of 13:05, 6 February 2011
Welcome to my new webpage (Nov-29-2010) Construction area.
Direct-sampling algorithm for ideal bosons in a trap (see article with M. Holzmann). Adapted for interacting bosons, this algorithm was used in a variety of articles.
Event-chain Monte Carlo algorithm for hard spheres and related systems (see article with E. P. Bernard and D. B. Wilson)
Exact diagonalization algorithm for Dynamical mean field theory (see article with M. Caffarel). This algorithm has been instrumental in our discovery of a first-order Mott transition in the Hubbard model in infinite dimensions. Much of our early work in the field is written up in our review with Georges, Kotliar, and Rozenberg
Rejection-free cluster algorithm for dimers (see article with R. Moessner). This algorithm was used for our discovery of a critical phase in three-dimensional dimer models (paper with Huse, Sondhi, and Moessner). Note that dimers flip about a symmetry axis between one valid configuration and another.
Werner Krauth Laboratoire de Physique Statistique École normale supérieure 24 rue Lhomond 75231 Paris Cedex 05 France Tel +33 (0) 44 32 25 50
