Non-ergodic Brownian oscillator
POSTER
Abstract
We consider an open (Brownian) classical harmonic oscillator
in contact with a non-Markovian thermal bath and described by the generalized Langevin equation.
When the bath's spectrum has a finite upper cutoff frequency,
the oscillator may have ergodic and non-ergodic configurations.
In ergodic configurations (when exist, they correspond to lower oscillator frequencies)
the oscillator demonstrates conventional thermalization, i.e. relaxation to thermal equilibrium with the bath.
In non-ergodic configurations (which correspond to higher oscillator frequencies)
the oscillator does not thermalize, but relaxes to a non-equilibrium
stationary state.
For a specific dissipation kernel in the Langevin equation, we evaluate explicitly relevant relaxation functions,
which describe the time evolution and properties of non-equilibrium stationary states.
When the oscillator's frequency is switched from a lower value to higher one,
the oscillator may show parametric transitions from ergodic to non-ergodic configurations.
These transitions are shown to resemble phase transitions of the second kind.
in contact with a non-Markovian thermal bath and described by the generalized Langevin equation.
When the bath's spectrum has a finite upper cutoff frequency,
the oscillator may have ergodic and non-ergodic configurations.
In ergodic configurations (when exist, they correspond to lower oscillator frequencies)
the oscillator demonstrates conventional thermalization, i.e. relaxation to thermal equilibrium with the bath.
In non-ergodic configurations (which correspond to higher oscillator frequencies)
the oscillator does not thermalize, but relaxes to a non-equilibrium
stationary state.
For a specific dissipation kernel in the Langevin equation, we evaluate explicitly relevant relaxation functions,
which describe the time evolution and properties of non-equilibrium stationary states.
When the oscillator's frequency is switched from a lower value to higher one,
the oscillator may show parametric transitions from ergodic to non-ergodic configurations.
These transitions are shown to resemble phase transitions of the second kind.
Presenters
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Alex Plyukhin
Saint Anselm College
Authors
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Alex Plyukhin
Saint Anselm College