Characterising the disordered state of block copolymers: Bifurcations of localised states and self-replication dynamics

2011 ◽  
Vol 23 (2) ◽  
pp. 315-341 ◽  
Author(s):  
KARL B. GLASNER

Above the spinodal temperature for micro-phase separation in block co-polymers, asymmetric mixtures can exhibit random heterogeneous structure. This behaviour is similar to the sub-critical regime of many pattern-forming models. In particular, there is a rich set of localised patterns and associated dynamics. This paper clarifies the nature of the bifurcation diagram of localised solutions in a density functional model of A−B diblock mixtures. The existence of saddle-node bifurcations is described, which explains both the threshold for heterogeneous disordered behaviour as well the onset of pattern propagation. A procedure to generate more complex equilibria by attaching individual structures leads to an interwoven set of solution curves. This results in a global description of the bifurcation diagram from which dynamics, in particular self-replication behaviour, can be explained.

1999 ◽  
Vol 10 (08) ◽  
pp. 1531-1540 ◽  
Author(s):  
T. KAWAKATSU ◽  
M. DOI ◽  
R. HASEGAWA

Slow dynamics of complex domain structures in phase separating polymer systems is investigated with the use of the self-consistent field (SCF) dynamic density functional (DDF) technique where the free energy of the system is calculated using the path integral formalism of the polymer chain conformation. We apply this technique to micellization of block copolymers and to phase separation of polymer blends containing block copolymers as a compatibilizer. In order to study the late stage of the phase separation processes more efficiently, we adopt the so-called Ginzburg–Landau approach, where a phenomenological model free energy functional is used. Numerical results of this approach is quantitatively compared with the results of the SCF approach.


Nanomaterials ◽  
2021 ◽  
Vol 11 (9) ◽  
pp. 2382
Author(s):  
Omar Abou El Kheir ◽  
Marco Bernasconi

Chalcogenide GeSbTe (GST) alloys are exploited as phase change materials in a variety of applications ranging from electronic non-volatile memories to neuromorphic and photonic devices. In most applications, the prototypical Ge2Sb2Te5 compound along the GeTe-Sb2Te3 pseudobinary line is used. Ge-rich GST alloys, off the pseudobinary tie-line with a crystallization temperature higher than that of Ge2Sb2Te5, are currently explored for embedded phase-change memories of interest for automotive applications. During crystallization, Ge-rich GST alloys undergo a phase separation into pure Ge and less Ge-rich alloys. The detailed mechanisms underlying this transformation are, however, largely unknown. In this work, we performed high-throughput calculations based on Density Functional Theory (DFT) to uncover the most favorable decomposition pathways of Ge-rich GST alloys. The knowledge of the DFT formation energy of all GST alloys in the central part of the Ge-Sb-Te ternary phase diagram allowed us to identify the cubic crystalline phases that are more likely to form during the crystallization of a generic GST alloy. This scheme is exemplified by drawing a decomposition map for alloys on the Ge-Ge1Sb2Te4 tie-line. A map of decomposition propensity is also constructed, which suggests a possible strategy to minimize phase separation by still keeping a high crystallization temperature.


1996 ◽  
Vol 100 (4) ◽  
pp. 413-417 ◽  
Author(s):  
Alexey L. Yakovlev ◽  
Georgy M. Zhidomirov ◽  
Konstantin M. Neyman ◽  
Vladimir A. Nasluzov ◽  
Notker Rösch

1997 ◽  
Vol 119 (1-3) ◽  
pp. 245-251 ◽  
Author(s):  
Konstantin M. Neyman ◽  
Markus Staufer ◽  
Vladimir A. Nasluzov ◽  
Notker Rösch

2019 ◽  
Vol 10 (46) ◽  
pp. 6254-6259 ◽  
Author(s):  
Ellis Hancox ◽  
Evelina Liarou ◽  
James S. Town ◽  
Glen R. Jones ◽  
Siân A. Layton ◽  
...  

Fluoro-polyacrylic acid block copolymers with vary narrow dispersity are shown to have sub-2 nm domain sizes on phase separation.


2010 ◽  
Vol 114 (31) ◽  
pp. 13287-13294 ◽  
Author(s):  
Benjamí Martorell ◽  
Alena Kremleva ◽  
Sven Krüger ◽  
Notker Rösch

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