2015
DOI: 10.1039/c4sm02010c
|View full text |Cite
|
Sign up to set email alerts
|

Structural and microscopic relaxations in a colloidal glass

Abstract: The aging dynamics of a colloidal glass has been studied by multiangle dynamic light scattering, neutron spin echo, X-ray photon correlation spectroscopy and molecular dynamics simulations. The two relaxation processes, microscopic (fast) and structural (slow), have been investigated in an unprecedentedly wide range of time and length scales covering both ergodic and nonergodic regimes. The microscopic relaxation time remains diffusive at all length scales across the glass transition scaling with wavevector Q … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

5
23
1

Year Published

2015
2015
2020
2020

Publication Types

Select...
4
3

Relationship

1
6

Authors

Journals

citations
Cited by 40 publications
(29 citation statements)
references
References 57 publications
(78 reference statements)
5
23
1
Order By: Relevance
“…In these works the fast process is independent on both T and time, and is due to microscopic PRL 118, 225901 (2017) Selected for a Viewpoint in Physics P H Y S I C A L R E V I E W L E T T E R S week ending 2 JUNE 2017 interactions between a particle and the cage created by its nearest neighbors. This fast process reflects a diffusive particle motion and it is usually described by a single exponential decay (thus with a shape exponent ¼ 1) [21]. In contrast with those works, here we probe the stress response in the deep nonequilibrium glassy state, and we observe a completely different additional decoupling between two dynamical processes.…”
mentioning
confidence: 45%
See 1 more Smart Citation
“…In these works the fast process is independent on both T and time, and is due to microscopic PRL 118, 225901 (2017) Selected for a Viewpoint in Physics P H Y S I C A L R E V I E W L E T T E R S week ending 2 JUNE 2017 interactions between a particle and the cage created by its nearest neighbors. This fast process reflects a diffusive particle motion and it is usually described by a single exponential decay (thus with a shape exponent ¼ 1) [21]. In contrast with those works, here we probe the stress response in the deep nonequilibrium glassy state, and we observe a completely different additional decoupling between two dynamical processes.…”
mentioning
confidence: 45%
“…This behavior changes when T is decreased 20 − 30 K below T g (open symbols). There, we do observe the formation of a shoulder for intermediate times (∼30 min) which becomes more and more prominent upon cooling, resulting in an unexpectedly well-defined two-step decay in the deep glass.The relaxation spectra observed here, phenomenologically bear a striking resemblance to that usually observed in the density fluctuations in Lennard-Jones glasses [2,17], molecular supercooled liquids [18], and colloidal suspensions [19][20][21]. In these works the fast process is independent on both T and time, and is due to microscopic PRL 118, 225901 (2017) …”
mentioning
confidence: 57%
“…4. Previous studies agree on the existence of a typical dual waiting time dependence of the structural relaxation time τ [2,3,37,5,13,27]: an exponential waiting time dependence τ (t w ) ∼ e tw at small t w , in the cage forming regime [37], and a waiting time power law dependence τ (t w ) ∼ t α w with α ∼ 1 at larger t w , in the full aging regime [37]. While in the cage forming regime the dynamical behaviour is diffusive (τ (Q) ∼ Q −2 ) with stretched (β <1) intensity correlation functions, in the full aging regime the dynamics is no more diffusive but characterized by a τ (Q) ∼ Q −1 dependence with three different behaviours of the correlation functions depending on the history of the sample.…”
Section: Resultsmentioning
confidence: 96%
“…It has been attributed to the relaxation of internal stresses [2,39,40]. In between the cage forming and full aging regimes MD simulations [27] find, in spontaneously aged sample, stretched exponential curves and a relaxation time well described as τ (Q) ∼ Q −n with 1 < n < 2.…”
Section: Resultsmentioning
confidence: 96%
See 1 more Smart Citation