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Department of Physics, Kyung Hee University
제13차 열 및 통계물리 워크샵 Drift와 결함이 있는 계의 표면 거칠기 Sooyeon Yoon & Yup Kim Department of Physics, Kyung Hee University
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Background of this study
• Edward-Wilkinson Eq. • G. Pruessner (PRL 92, (2004)) v : drift velocity with Fixed Boundary Condition (FBC) Surface roughness L : system size h : the height of surface Family-Vicsek Scaling behavior EW universality class Anomalous exponents
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Motivation 1. What is the simple stochastic discrete surface growth model to describe the EW equaiton with drift and FBC ? • Numerical Integration • Toy models : Family model, Equilibrium Restricted Solid-On-Solid (RSOS) model … Stochastic analysis for the Langevin equation ( S.Y. Yoon & Yup Kim, JKPS 44, 538 (2004) ) 2. Application The effect of the defect and drift for the surface growth ?
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A stochastic analysis of continuum Langevin equation
for surface growths S.Y. Yoon & Yup Kim, JKPS 44, 538 (2004)) • Continuum Langevin Equation : • Fokker-Planck Equation : is the transition rate from H′ to H. • Master Equation : If we consider the deposition(evaporation) of only one particle at the unit evolution step. ( a is the lattice constant. ) (deposition) (evaporation)
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Model • Evolution rate on the site For the Edward-Wilkinson equation with drift, • Determine the evolution of the center point (x0=L/2) by the defect strength. x0=L/2 p x d (e ) d (e ) or
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Simulation Results Scaling Properties of the Surface Width
(FBC, p=0) (PBC, p=1)
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Analysis of the Interface Profile
~
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Crossover (EWanomalous roughening) according to the defect strength
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Phase transition of RSOS model with a defect site
: H.S.Song & J.M.Kim (Sae Mulli, 50, 221 (2005)) r : the distance from the center point P : defect strength P=0, facet Pc P=1, RSOS EW p=0 p=1
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G Application of the surface growth by the defect (Queuing problem)
. . ( a : lattice constant ) . ( : particle density ) G slowly go out ! fast get in !
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EW (p0) Anomalous roughening (p=0)
Conclusion We studied the phase transition of the stochastic model which satisfies the Edward-Wilkinson equation with a drift and a defect on the 1-dimensional system. 1. The scaling exponents are changed by the drift and the perfect defect. Anomalous exponents 2. Crossover EW (p0) Anomalous roughening (p=0) 3. Application to the queuing phenomena ( at p=0 : perfect defect ).
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