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| 1 | Suppression of Chaos by Resonant parametric perturbations显示文摘 | Lima R Pettini M | 1990 | Phys Rev A1990，，41： | 1 |
| 2 | Chaotic behavior in nonlinear Hamiltonian systems and equilibrium statistical mechanics显示文摘 | Roberto Livi Marco Pettini Stefano Ruffo Angelo Vulpiani | 1987 | Journal of Statistical Physics1987，，3： | 1 |
| 3 | Cytogenetic genotoxicinvestigation in peripheral blood lymphocytes of subjects withdental composite restorative filling materials 显示文摘 | Pettini F Savino M Corsalini M | 2015 | J Biol RegulHomeost Agents2015，29，1： | 1 |
| 4 | Epidemiology, associated factors and outcomes of ICU - acquired infections caused by Gram - negative bacteria in critically ill patients: an observational, retrospective study显示文摘 | Chelazzi C Pettini E Villa G | 2015 | BMC Anesthesiology2015，15，1： | 1 |
| 5 | Suppression of chaos by resonant parametric perturbations显示文摘 | Lima R Pettini M | 1990 | Physical Review A1990，41，2： | 1 |
| 6 | Experimental evidence of suppression of chaos by resonant parametric perturbations显示文摘 | Fronzoni L Geocondo M Pettini M | 1991 | Physical Review A1991，43，12： | 1 |
| 7 | Suppressing of chaos by resonant parameter perturbations 显示文摘 | LIMA R PETTINI M | 1990 | Physical Review A1990，41，2： | 1 |
| 8 | Suppression of chaos by resonant parametric perturbations显示文摘 | LIMA R PETTINI M | 1990 | Physical Review A1990，41，2： | 1 |
| 9 | Primary activation of antigen-specific naive CD4 ^+ and CDs^+ T cells following intranasal vaccination with recombinant bacteria显示文摘 | Ciabattini A Pettini E Andersen P | 2008 | Infect Immun2008，76，12： | 1 |
| 10 | Geometric approach to Hamiltonian dynamics and statistical mechanics 显示文摘 | Casetti L Pettini M Cohen E G D | 2000 | Physics Reports2000，337，3： | 1 |
| 11 | Suppression of chaos by resonant parametric Perturbations显示文摘 | Lima B Pettini M | 1990 | Phys Rev1990，41，： | 1 |
| 12 | Suppression of chaos by resonant parametric perturbations 显示文摘 | Lima B Pettini M | 1990 | Physical Review A1990，41，2： | 1 |
| 13 | Suppression of Chaos by ResonantParametric Perturbations显示文摘 | Lima B Pettini M | 1990 | Phys Rev A1990，41，： | 1 |
| 14 | Suppression of chaos by resonant parametric perturbations显示文摘 | Lima R Pettini M | 1990 | Physical Review A1990，，41： | 1 |
| 15 | Suppression of chaos by resonant parametric perturbations显示文摘 | PETTINI M | 1990 | IEEE Trans on Circ and Syst Phys Rev(A)1990，41，2： | 1 |
| 16 | Suppression of chaos by resonant parametric perturbations显示文摘 | Lima R Pettini M | 1990 | Physical Review A1990，41，2： | 1 |
| 17 | Suppression of chaos by resonant parametric perturbations 显示文摘 | Lima R Pettini M | 1990 | Physical Review A1990，41，2： | 1 |
| 18 | Suppression of chaos by resonant parametric perturbations显示文摘 | LIMA R PETTINI M | 1990 | Phys Rev A1990，41，2： | 1 |
| 19 | Geometric approach to Hamiltonian dynamics and statistical mechanics显示文摘 | Casetti L Pettini M Cohen E G D | 2000 | Physics Reports2000，337，3： | 1 |
| 20 | Tight-binding models for ultracold atoms in optical lattices:general formulation and applications显示文摘Tight-binding models for ultracold atoms in optical lattices can be properly defined by using the concept of maximally localized Wannier functions for composite bands. The basic principles of this approach are reviewed here, along with different applications to lattice potentials with two minima per unit cell, in one and two spatial dimensions. Two independent methods for computing the tight-binding coefficients—one ab initio, based on the maximally localized Wannier functions, the other through analytic expressions in terms of the energy spectrum—are considered. In the one dimensional case, where the tight-binding coefficients can be obtained by designing a specific gauge transformation, we consider both the case of quasi resonance between the two lowest bands, and that between s and p orbitals. In the latter case, the role of the Wannier functions in the derivation of an effective Dirac equation is also reviewed. Then, we consider the case of a two dimensional honeycomb potential, with particular emphasis on the Haldane model, its phase diagram, and the breakdown of the Peierls substitution. Tunable honeycomb lattices, characterized by movable Dirac points, are also considered. Finally, general considerations for dealing with the interaction terms are presented. | Michele Modugno Julen Ibanez-Azpiroz Giulio Pettini | 2016 | Science China(Physics,Mechanics & Astronomy)2016，59，6： | 1 |
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