SP Seminar @SISSA Via Bonomea 265 - Thursday 21 November at 10:30 am - Uwe TAUBER
CM Section
cm at ictp.it
Fri Nov 15 14:08:23 CET 2019
Kindly note UNUSUAL DAY and TIME
Joint ICTP/SISSA Statistical Physics Seminar
Thursday 21 November at 10:30 a.m.
venue: SISSA, Via Bonomea 265
Speaker: Uwe TAUBER
Virginia Tech, U.S.A.
Title: Temperature Interfaces in the Katz-lebowitz-Spohn
Driven Lattice Gas
Abstract:
We explore the intriguing spatial patterns that emerge in a
two-dimensional spatially inhomogeneous Katz-Lebowitz-Spohn (KLS) driven
lattice gas with attractive nearest-neighbor interactions. The domain is
split into two regions with hopping rates governed by different
temperatures T > T_c and T_c, respectively, where T_c indicates the
critical temperature for phase ordering, and with the temperature
boundaries oriented perpendicular to the drive. In the hotter region,
the system behaves like the (totally) asymmetric exclusion processes
(TASEP), and experiences particle blockage in front of the interface to
the critical region. To explain this particle density accumulation near
the interface, we have measured the steady-state current in the KLS
model at T > T_c and found it to decay as 1/T. In analogy with TASEP
systems containing "slow" bonds, transport in the high-temperature
subsystem is impeded by the lower current in the cooler region, which
tends to set the global stationary particle current value. This blockage
is induced by the extended particle clusters, growing logarithmically
with system size, in the critical region. We observe the density
profiles in both high-and low-temperature subsystems to be similar to
the well-characterized coexistence and maximal-current phases in (T)ASEP
models with open boundary conditions, which are respectively governed by
hyperbolic and trigonometric tangent functions. Yet if the lower
temperature is set to T_c, we detect marked fluctuation corrections to
the mean-field density profiles, e.g., the corresponding critical KLS
power law density decay near the interfaces into the cooler region. If
the temperature interface is aligened parallel to the drive, we observe
the cooler region to act as an absorbing sink for particle transport,
with blockages emerging at the subsystem boundaries.
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