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Driven, underdamped Frenkel-Kontorova model on a quasiperiodic substrate
A Vanossi1, J Röder, A R Bishop
1Theoretical Division and Center for Nonlinear Studies, Los Alamos National Laboratory, Los Alamos, NM 87545, USA.
Summary
Investigating atom chains with incommensurate length scales reveals that zero static friction is possible when scales relate via the spiral mean. Quadratic irrationals like the golden mean always result in nonzero static friction.
Area of Science:
- Condensed matter physics
- Statistical mechanics
- Nonlinear dynamics
Background:
- Underdamped dynamics of atomic chains are crucial for understanding friction and transport phenomena.
- Quasiperiodic potentials introduce complex behaviors in driven systems.
- Incommensurate length scales lead to rich phenomena in condensed matter systems.
Purpose of the Study:
- To investigate the conditions under which static friction can be zero in a driven atomic chain system.
- To explore the role of incommensurate length scales and their mathematical relationships on static friction.
- To understand the depinning mechanisms and steady states in such systems.
Main Methods:
- Numerical simulations of underdamped atomic chains.
- Analysis of system dynamics under dc driving force and quasiperiodic substrate potential.
- Theoretical considerations based on standard map theory.
Main Results:
- Zero static friction is achievable when three mutually incommensurate length scales are related by the spiral mean (cubic irrational).
- Static friction remains nonzero for all interaction strengths when length scales are related by the golden mean (quadratic irrational).
- Zero static friction is generally possible for incommensurate ratios, but not for quadratic irrationals or commensurable scales.
Conclusions:
- The mathematical nature of the ratio between length scales dictates the possibility of zero static friction.
- Systems with quadratic irrational or commensurable length scales exhibit always nonzero static friction.
- Depinning mechanisms and steady states are influenced by the interplay of driving force, substrate potential, and interparticle interactions.