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Title: Dodecagonal quasicrystalline order in a diblock copolymer melt

Abstract

We report the discovery of a dodecagonal quasicrystalline state (DDQC) in a sphere (micelle) forming poly(isoprene-b-lactide) (IL) diblock copolymer melt, investigated as a function of time following rapid cooling from above the order–disorder transition temperature (TODT = 66 °C) using small-angle X-ray scattering (SAXS) measurements. Between TODT and the order–order transition temperature TOOT = 42 °C, an equilibrium body-centered cubic (BCC) structure forms, whereas below TOOT the Frank–Kasper σ phase is the stable morphology. At T < 40 °C the supercooled disordered state evolves into a metastable DDQC that transforms with time to the σ phase. The times required to form the DDQC and σ phases are strongly temperature dependent, requiring several hours and about 2 d at 35 °C and more than 10 and 200 d at 25 °C, respectively. Remarkably, the DDQC forms only from the supercooled disordered state, whereas the σ phase grows directly when the BCC phase is cooled below TOOT and vice versa upon heating. A transition in the rapidly supercooled disordered material, from an ergodic liquid-like arrangement of particles to a nonergodic soft glassy-like solid, occurs below ~40 °C, coincident with the temperature associated with the formation of the DDQC. We speculate that thismore » stiffening reflects the development of particle clusters with local tetrahedral or icosahedral symmetry that seed growth of the temporally transient DDQC state. Here, this work highlights extraordinary opportunities to uncover the origins and stability of aperiodic order in condensed matter using model block polymers.« less

Authors:
 [1];  [2];  [1]
  1. Univ. of Minnesota, Minneapolis, MN (United States)
  2. Rensselaer Polytechnic Inst., Troy, NY (United States)
Publication Date:
Research Org.:
Argonne National Laboratory (ANL), Argonne, IL (United States)
Sponsoring Org.:
USDOE Office of Science (SC), Basic Energy Sciences (BES). Scientific User Facilities Division; National Science Foundation (NSF)
OSTI Identifier:
1256354
Grant/Contract Number:  
AC02-06CH11357; 1104368
Resource Type:
Accepted Manuscript
Journal Name:
Proceedings of the National Academy of Sciences of the United States of America
Additional Journal Information:
Journal Volume: 113; Journal Issue: 19; Journal ID: ISSN 0027-8424
Publisher:
National Academy of Sciences
Country of Publication:
United States
Language:
ENGLISH
Subject:
37 INORGANIC, ORGANIC, PHYSICAL, AND ANALYTICAL CHEMISTRY; quasicrystals; Frank–Kasper phases; block polymers

Citation Formats

Gillard, Timothy M., Lee, Sangwoo, and Bates, Frank S. Dodecagonal quasicrystalline order in a diblock copolymer melt. United States: N. p., 2016. Web. doi:10.1073/pnas.1601692113.
Gillard, Timothy M., Lee, Sangwoo, & Bates, Frank S. Dodecagonal quasicrystalline order in a diblock copolymer melt. United States. https://doi.org/10.1073/pnas.1601692113
Gillard, Timothy M., Lee, Sangwoo, and Bates, Frank S. Tue . "Dodecagonal quasicrystalline order in a diblock copolymer melt". United States. https://doi.org/10.1073/pnas.1601692113. https://www.osti.gov/servlets/purl/1256354.
@article{osti_1256354,
title = {Dodecagonal quasicrystalline order in a diblock copolymer melt},
author = {Gillard, Timothy M. and Lee, Sangwoo and Bates, Frank S.},
abstractNote = {We report the discovery of a dodecagonal quasicrystalline state (DDQC) in a sphere (micelle) forming poly(isoprene-b-lactide) (IL) diblock copolymer melt, investigated as a function of time following rapid cooling from above the order–disorder transition temperature (TODT = 66 °C) using small-angle X-ray scattering (SAXS) measurements. Between TODT and the order–order transition temperature TOOT = 42 °C, an equilibrium body-centered cubic (BCC) structure forms, whereas below TOOT the Frank–Kasper σ phase is the stable morphology. At T < 40 °C the supercooled disordered state evolves into a metastable DDQC that transforms with time to the σ phase. The times required to form the DDQC and σ phases are strongly temperature dependent, requiring several hours and about 2 d at 35 °C and more than 10 and 200 d at 25 °C, respectively. Remarkably, the DDQC forms only from the supercooled disordered state, whereas the σ phase grows directly when the BCC phase is cooled below TOOT and vice versa upon heating. A transition in the rapidly supercooled disordered material, from an ergodic liquid-like arrangement of particles to a nonergodic soft glassy-like solid, occurs below ~40 °C, coincident with the temperature associated with the formation of the DDQC. We speculate that this stiffening reflects the development of particle clusters with local tetrahedral or icosahedral symmetry that seed growth of the temporally transient DDQC state. Here, this work highlights extraordinary opportunities to uncover the origins and stability of aperiodic order in condensed matter using model block polymers.},
doi = {10.1073/pnas.1601692113},
journal = {Proceedings of the National Academy of Sciences of the United States of America},
number = 19,
volume = 113,
place = {United States},
year = {Tue Apr 26 00:00:00 EDT 2016},
month = {Tue Apr 26 00:00:00 EDT 2016}
}

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