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(2002)
and F
N. Busch, N. Vinnichenko, A. Waterman, C. Beard, R. Stewart, R. Scotti (1969)
Waves and TurbulenceRadio Science, 4
(1984)
Chemical Osillation
We take "interface" or "height" equation in the restricted sense that physics is invariant under global height shifts h(x, t) → h(x, t) + const
C. Rhodes, Eugene Stanley (1996)
Fractal Concepts in Surface GrowthZeitschrift für Physikalische Chemie, 193
By defining l ocal width as w 2 (x0) = D P xˆh (x, t) −hx 0˜2 /x0 E we have W = w(x0 = L)
(1995)
Politi and C . Misbah
(2006)
Phys
(2000)
The stochastic version of this 2d equation was previously derived in the context of amorphous thin film growth, see
A local evolution equation for one-dimensional interfaces is derived in the context of erosion by ion beam sputtering. We present numerical simulations of this equation which show interrupted coarsening in which an ordered cell pattern develops with constant wavelength and amplitude at intermediate distances, while the profile is disordered and rough at larger distances. Moreover, for a wide range of parameters the lateral extent of ordered domains ranges up to tens of cells. We also provide analytical estimates for the stationary pattern wavelength and mean growth velocity.
Physical Review E – American Physical Society (APS)
Published: Nov 1, 2006
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