On the Mechanism of Soft Self‐Assembly from Melt: The Ubiquitous Heat Capacity Hump and Spontaneous Melt Chirality

Y Yi‐nan Xue (Shaanxi International Research Center for Soft Matter, State Key Laboratory for Mechanical Behavior of Materials Xi'an Jiaotong University Xi'an 710049 China) X Xiang‐bing Zeng (School of Chemical Materials and Biological Engineering University of Sheffield Sheffield S1 3JD UK) B Bo‐wen Wu (Shaanxi International Research Center for Soft Matter State Key Laboratory for Mechanical Behaviour of Materials Xi'an Jiaotong University Xi'an 710049 China) Y Ya‐xin Li (School of Chemistry and Chemical Engineering Henan University of Technology Zhengzhou 450001 China) L Liliana Cseh (Romanian Academy) S Shu‐Gui Yang (Shaanxi International Research Center for Soft Matter, State Key Laboratory for Mechanical Behavior of Materials Xi'an Jiaotong University Xi'an 710049 China) J Jie Liu G Gillian A. Gehring (School of Mathematical and Physical Sciences University of Sheffield Sheffield S3 7RH UK) F Feng Liu G Goran Ungar (Shaanxi International Research Center for Soft Matter, State Key Laboratory for Mechanical Behaviour of Materials)

Abstract

Abstract We investigate two unusual phenomena in self‐assembly of anisotropic molecules from isotropic (Iso) melt: a heat‐capacity ( C p ) maximum and spontaneous formation of the recently discovered chiral liquid (Iso*). Based on experiments on new nonchiral monomers, dimers, and polymers, we construct a statistical theory that shows why many complex meso‐structures form in two stages: continuous equilibrium growth of nano‐clusters in melt through strong interactions, causing the C p ‐maximum, followed by establishment of positional long‐range order (LRO) through a weak first‐order transition. We also show why many achiral compounds additionally form an intermediate chiral Iso* liquid through what we find is a second‐order transition. We propose that the first process is equivalent to “supramolecular polymerization” in solutions, where the lack of intercluster interaction rules out LRO. Furthermore, we argue that separation into a broad and a sharp transition is universal in condensed matter where strong interactions by themselves cannot lead to LRO, either because the clusters are 1D or due to strong frustration. Clusters must first grow to critical size when, at T c , the combined weak interactions reach ∼k B T c , prompting LRO formation. A situation similar to that in soft self‐assembly is seen in spin ordering in magnetic crystals, but only near 0 K.

Article Details

Volume / Issue Vol. 64, Issue 28
Published July 07, 2025
ISSN 1433-7851
Publisher Wiley

Journal Info

Angewandte Chemie International Edition

Wiley

ISSN: 1433-7851 Physical Sciences

Authors (10)

Y

Yi‐nan Xue

Shaanxi International Research Center for Soft Matter, State Key Laboratory for Mechanical Behavior of Materials Xi'an Jiaotong University Xi'an 710049 China

X

Xiang‐bing Zeng

School of Chemical Materials and Biological Engineering University of Sheffield Sheffield S1 3JD UK

B

Bo‐wen Wu

Shaanxi International Research Center for Soft Matter State Key Laboratory for Mechanical Behaviour of Materials Xi'an Jiaotong University Xi'an 710049 China

Y

Ya‐xin Li

School of Chemistry and Chemical Engineering Henan University of Technology Zhengzhou 450001 China

L

Liliana Cseh

Romanian Academy

S

Shu‐Gui Yang

Shaanxi International Research Center for Soft Matter, State Key Laboratory for Mechanical Behavior of Materials Xi'an Jiaotong University Xi'an 710049 China

J

Jie Liu

G

Gillian A. Gehring

School of Mathematical and Physical Sciences University of Sheffield Sheffield S3 7RH UK

F

Feng Liu

G

Goran Ungar

Shaanxi International Research Center for Soft Matter, State Key Laboratory for Mechanical Behaviour of Materials