activity
20002009
most citedIsing transition driven by frustration in a 2D classical model with SU(2) symmetry

103 citations · 381 across the 17 of their papers we have counts for

collaborators

17 papers

cond-mat.str-el2009★ 1 cited

Variational wave functions for frustrated magnetic models

Federico Becca, Luca Capriotti, Alberto Parola +1

Variational wave functions containing electronic pairing and suppressed charge fluctuations (i.e., projected BCS states) have been proposed as the paradigm for disordered magnetic…

cond-mat.str-el2007★ 8 cited

Exotic gapless spectrum induced by frustration in quantum antiferromagnets

Federico Becca, Luca Capriotti, Alberto Parola +1

We show strong numerical evidence in favor of an unexpected virtually gapless spectrum, with edge states localized at the boundaries, in frustrated spin-1/2 antiferromagnetic ladde…

cond-mat.str-el2005

The resonating valence bond wave functions in quantum antiferromagnets

Alberto Parola, Sandro Sorella, Federico Becca +1

Projected-BCS wave functions have been proposed as the paradigm for the understanding of disordered spin states (spin liquids). Here we investigate the properties of these wave fun…

cond-mat.str-el2005

Quantum Heisenberg antiferromagnets: a survey of the activity in Firenze

Umberto Balucani, Luca Capriotti, Alessandro Cuccoli +5

Over the years the research group in Firenze has produced a number of theoretical results concerning the statistical mechanics of quantum antiferromagnetic models, which range from…

cond-mat.stat-mech2004★ 26 cited

Dissipation-driven phase transition in 2D Josephson arrays

Luca Capriotti, Alessandro Cuccoli, Andrea Fubini +2

We analyze the interplay of dissipative and quantum effects in the proximity of a quantum phase transition. The prototypical system is a resistively shunted two-dimensional Josephs…

cond-mat.str-el2004★ 53 cited

Low temperature broken symmetry phases of spiral antiferromagnets

Luca Capriotti, Subir Sachdev

We study Heisenberg antiferromagnets with nearest- (J1) and third- (J3) neighbor exchange on the square lattice. In the limit of large spin S, there is a zero temperature (T) Lifsh…