2001
DOI: 10.1007/s101890170079
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Glassy dynamics of simulated polymer melts: Coherent scattering and van Hove correlation functions

Abstract: Whereas the first part of this paper dealt with the relaxation in the β-regime, this part investigates the final relaxation (α-relaxation) of a simulated polymer melt consisting of short non-entangled chains in the supercooled state above the critical temperature Tc of ideal mode-coupling theory (MCT). The temperature range covers the onset of a two-step relaxation behaviour down to a temperature merely 2% above Tc. We monitor the incoherent intermediate scattering function as well as the coherent intermediate… Show more

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Cited by 54 publications
(101 citation statements)
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References 69 publications
(163 reference statements)
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“…III A), i.e., it is connected to the overall size of the molecule. It is interesting to note that similar unusual peaks were found in a model for polymer around the intermediate wavenumber q = 2π/R g , where R g denotes the radius of gyration [53]: in this wavenumber regime, a shoulder is discernible in the critical nonergodicity parameters f c q , and peaks are observable in the inverse of the critical amplitudes 1/h q , the α-relaxation times τ q , and the stretching exponents β q of the correlators which correspond to φ N q (t) in the present paper. In particular, the ratio τ q /τ qmax of the α-relaxation times at q ≈ 2π/R g for this model exhibits the same temperature dependence as the one shown in Fig.…”
Section: Summary and Concluding Remarkssupporting
confidence: 66%
“…III A), i.e., it is connected to the overall size of the molecule. It is interesting to note that similar unusual peaks were found in a model for polymer around the intermediate wavenumber q = 2π/R g , where R g denotes the radius of gyration [53]: in this wavenumber regime, a shoulder is discernible in the critical nonergodicity parameters f c q , and peaks are observable in the inverse of the critical amplitudes 1/h q , the α-relaxation times τ q , and the stretching exponents β q of the correlators which correspond to φ N q (t) in the present paper. In particular, the ratio τ q /τ qmax of the α-relaxation times at q ≈ 2π/R g for this model exhibits the same temperature dependence as the one shown in Fig.…”
Section: Summary and Concluding Remarkssupporting
confidence: 66%
“…It is interesting to note that a similar unusual peak was found in a model for polymer around wavenumbers close to the inverse radius of gyration [21]. In Ref.…”
supporting
confidence: 69%
“…These type of binary mixtures exhibit unusual relaxation features which challenge standard pictures for structural dynamic arrest in glass-forming liquids and colloidal systems. Differently from the usual two-step increase and decay for, respectively, mean squared displacements and dynamic correlators [1,2,3,4,5], the latters do not exhibit a defined plateau at intermediate times between the microscopic and diffusive regimes [6,7,8]. This result suggests a softer character for the collective caging mechanism -i.e., the temporary trapping of each particle by its neighbors.…”
Section: Introductionmentioning
confidence: 68%
“…For the case x small = 0.1 (Fig. 5a), A-A correlations display the standard behavior observed for liquid-glass transitions [1,2,3,4,5]. After the initial transient regime, F AA (q, t) shows a first decay to a plateau.…”
Section: Density-density Correlatorsmentioning
confidence: 78%