2015
DOI: 10.1016/j.colsurfa.2015.06.001
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Non-diffusive dynamics in a colloidal glass: Aging versus rejuvenation

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Cited by 13 publications
(12 citation statements)
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“…(6). It evolves from an exponential behaviour τ = τ 0 exp( D t t w t ∞ w −t w ) (3,5,6,9) where t w drives the system out of equilibrium and t ∞ w sets the apparent divergence (56,57), to a slower than Arrhenius dependence with increasing t w . Fig.…”
Section: Resultsmentioning
confidence: 99%
“…(6). It evolves from an exponential behaviour τ = τ 0 exp( D t t w t ∞ w −t w ) (3,5,6,9) where t w drives the system out of equilibrium and t ∞ w sets the apparent divergence (56,57), to a slower than Arrhenius dependence with increasing t w . Fig.…”
Section: Resultsmentioning
confidence: 99%
“…[8]. It changes from a VFT behaviour τ = τ 0 exp( D t t w t ∞ w −t w ) [5,7,8,12] where t w replaces 1/T and t ∞ w sets the apparent divergence [66,67], to a slower than Arrhenius behaviour with increasing t w . Moreover in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…the slowing down of the dynamics achieved by varying packing fraction [47,69], waiting time [5,7,8,12] or temperature [22,23] is accompanied by a super Arrhenius increase, typically VFT, of the structural relaxation time followed by a slower than Arrhenius or an Arrhenius behaviour. Thus the existence of two different dynamical regimes is a general feature of soft colloids, hard colloids and structural glasses.…”
Section: Resultsmentioning
confidence: 99%
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“…Each of these factors can affect the interparticle interactions and consequently the viscoelastic properties. For instance, the presence of charged species has been shown to alter the liquid to gel transition in laponite suspensions [32][33][34]. Suspensions and gels of cellulose nanocrystals are a compelling case in point, as they display a wide variety of solvent-mediated interparticle interactions including van der Waals attraction, hydrogen bonding and electrostatic repulsion [35,36].…”
Section: Introductionmentioning
confidence: 99%