TY - JOUR
T1 - Frenkel-Kontorova model
T2 - Crossover from the classical to the quantum mechanical
AU - Hu, Bambi
AU - Li, Baowen
PY - 1999
Y1 - 1999
N2 - The Frenkel-Kontorova (FK) model describes a chain of atoms connected by springs subject to an external potential. This simple classical model exhibits a wealth of complex behavior. It has also found applications in many condensed matter systems such as charge density waves, magnetic spirals, modulated phases and tribology. However, an in-depth understanding of some of these problems, for example, tribology in the nano-regime, demands an understanding of its quantum mechanical behavior. To achieve this goal, we use a squeezed-state approach first used in quantum optics. We found that quantum fluctuations renormalize the standard map, which governs the classical behavior of the FK model, to a sawtooth map. This result is borne out by Monte-Carlo simulations. We also found that the ground state wave function changes from an extended state to a localized state when the coupling constant increases. Although quantum fluctuations largely smear the transition by breaking of analyticity observed in the classical case, the remnant of this transition is still discernible.
AB - The Frenkel-Kontorova (FK) model describes a chain of atoms connected by springs subject to an external potential. This simple classical model exhibits a wealth of complex behavior. It has also found applications in many condensed matter systems such as charge density waves, magnetic spirals, modulated phases and tribology. However, an in-depth understanding of some of these problems, for example, tribology in the nano-regime, demands an understanding of its quantum mechanical behavior. To achieve this goal, we use a squeezed-state approach first used in quantum optics. We found that quantum fluctuations renormalize the standard map, which governs the classical behavior of the FK model, to a sawtooth map. This result is borne out by Monte-Carlo simulations. We also found that the ground state wave function changes from an extended state to a localized state when the coupling constant increases. Although quantum fluctuations largely smear the transition by breaking of analyticity observed in the classical case, the remnant of this transition is still discernible.
UR - http://www.scopus.com/inward/record.url?scp=0033471872&partnerID=8YFLogxK
M3 - Journal article
AN - SCOPUS:0033471872
SN - 0374-4884
VL - 34
SP - S138-S142
JO - Journal of the Korean Physical Society
JF - Journal of the Korean Physical Society
IS - SUPPL. 2
ER -