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D.D. Vvedensky, S. Clarke, K.J. Hugill, A.K. Myers-Beaghton, and M.R. Wilby, in Kinetics of Ordering and Growth at Surfaces, edited by M.G. Lagally (Plenum Press, New York, 1990), p. 297.
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A direct integration of Eq. (1), with the nonlinear terms ∇(∇h(Formula presented) and (Formula presented)(∇h(Formula presented), gives the EW exponent Β≈1/4 [J.M. Kim and S. Das, Sarma, Phys. Rev. E 51, 1889 (1995)], in agreement with renormalization-group analysis of S. Das Sarma and R. Kotlyar, ibid. 50, R4275 (1994), according to which a Laplacian term appears upon renormalization (cf. also the discussion in Ref. 1).
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However, this type of anomalous scaling that appears, e.g., for the linear equation (cf. the paper by Amar
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Note that unusual scaling of G(r, t), which occurs if ζ>1, was first noted by J.G. Amar, P.-M. Lam and F. Family, Phys. Rev. E 47, 3242 (1993) and H. Leschhorn and L.-H. Tang, Phys. Rev. Lett. 70, 2973 (1993). However, this type of anomalous scaling that appears, e.g., for the linear equation (cf. the paper by Amar et. al), does not lead to anomalous scaling of the structure factor and is thus rather different from the anomalous scaling considered in Refs. 13 and 29 (cf. the discussion in Ref. 1).
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We stress that, in the present paper (Sec. IV), a FD model with random deposition of incoming particles (without any incorporation search) is used
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We used the algorithm for the relaxation of incoming particles that is similar to the one employed earlier in simulations of the FD model, cf. S. Clarke, M.R. Wilby and D.D. Vvedensky, Surf. Sci. 255, 91 (1991). We stress that, in the present paper (Sec. IV), a FD model with random deposition of incoming particles (without any incorporation search) is used.
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M. Siegert, Phys. Rev. E (to be published).
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D. E. Wolf, in Scale Invariance, Interfaces, and Non-Equilibrium Dynamics, edited by A. McKane, M. Droz, J. Vannimenus, and D. Wolf (Plenum, New York, 1995), p. 215.
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T. Shitara, D.D. Vvedensky, M.R. Wilby, J. Zhang, J.H. Neave and B.A. Joyce, Phys. Rev. B 46, 6815 (1992).
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T. Shitara, D.D. Vvedensky, M.R. Wilby, J. Zhang, J.H. Neave and B.A. Joyce, Phys. Rev. B 46, 6825 (1992).
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53
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0347884938
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Note that the dependence G(1, t)∝logt has been observed in an experimental study of Si/Si(111) growth [H.-N. Yang, G.-C. Wang, and T.-M. Lu, Phys. Rev. Lett. 73, 2348 (1994)].
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For recent reviews of experiments on kinetic roughening see, e.g., the review paper G. Palasantzas and J. Krim, Int. J. Mod. Phys. B 9, 599 (1995), the work of Krug (Ref. 1), or the book of Barabási and Stanley (Ref. 2).
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