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note
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Note that modest adaptations permit us to incorporate the hydrodynamic effect. We have illustrated the method for homopolymer kinetics in a previous work in Ref. [36].
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66
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note
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3. However, this is a delicate question that requires a separate study for heteropolymers.
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67
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85088228974
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note
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m . This expresses the inversion symmetry of Ref. [35] and allows one to establish the correct correspondence of a ring with N units to an open chain with N/2 units (see Ref. [36] for more detail).
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70
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5644236942
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note
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3. The latter is considerably smaller than the former for the whole range of considered parameters, justifying the use of the weak-disorder expansion.
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note
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q(t) exhibit the characteristic growth exponents similar to the treatments of spinodal decomposition by Cahn et al., but for special q's, not for special 3d momenta k. That is why we call this phenomenon the spinodal decomposition in the internal metric of the chain. This is discussed in more detail in Refs. [28,36].
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73
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note
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q similarly to our heteropolymer work [35]. Thus a change of Ψ accompanied by fast changes of large-q modes (small distances along the chain) corresponds to the microphase separation, while a change of Ψ together with the small-q modes describes the overall restructuring of the hydrophobic and hydrophilic units. One can have a better feeling about both processes by using the visualization of individual conformations in the Monte Carlo method [29].
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75
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H. Sompolinsky and A. Zippelius, Phys. Rev. Lett. 45, 359 (1981); Phys. Rev. B 25, 274 (1982).
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80
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note
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1 describes the mean distance between two nearest neighbors along the chain. From Fig. 8 one can see that in the folded state [curve (e)] this differs only in approximately 1.3 times compared to the ideal coil, for which that distance is equal to 1 in our units by definition.
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