TY - JOUR
T1 - Glass Transition Behavior in Thin Polymer Films Covered with a Surface Crystalline Layer
AU - Zuo, Biao
AU - Liu, Yue
AU - Liang, Yongfeng
AU - Kawaguchi, Daisuke
AU - Tanaka, Keiji
AU - Wang, Xinping
N1 - Funding Information:
We gratefully acknowledge the support from the National Natural Science Foundation of China (21374104, 21504081, and 21674100), the Natural Science Foundation of Zhejiang Province (LQ16B040001), Young Researchers Foundation of Key Laboratory of Advanced Textile Materials and Manufacturing Technology, Zhejiang Sci-Tech University (2015QN04), JSPS KAKENHI, Grant-in-Aids for Scientific Research (A) (15H02183), and JST SENTANKEISOKU (13A0004). GIWAXD measurements were performed at BL03XU (Frontier Softmaterial Beamline (FSBL)) in SPring-8 with the approval of the Japan Synchrotron Radiation Research Institute (JASRI) (Proposal: 2016A7225).
Publisher Copyright:
© 2017 American Chemical Society.
Copyright:
Copyright 2018 Elsevier B.V., All rights reserved.
PY - 2017/3/14
Y1 - 2017/3/14
N2 - Thin amorphous poly(ethylene terephthalate) (PET) films covered with/without a crystallized surface layer were prepared onto silicon wafers. In the former and latter cases, the surface mobility in the film was depressed and enhanced, respectively. The glass transition temperature (Tg) of the amorphous PET film decreased with the reduction of the film thickness, exhibiting a remarkable nanoconfinement effect. However, once the surface region of the thin film was crystallized, or frozen in terms of the segmental motion, Tg of the films recovered to that of the bulk. Concurrently, the apparent activation energy of the segmental motion in the surface-crystallized film was in good accordance with the bulk value as well. These results make it clear that the mobility in the surface region plays an essential role in the glass transition of the thin films.
AB - Thin amorphous poly(ethylene terephthalate) (PET) films covered with/without a crystallized surface layer were prepared onto silicon wafers. In the former and latter cases, the surface mobility in the film was depressed and enhanced, respectively. The glass transition temperature (Tg) of the amorphous PET film decreased with the reduction of the film thickness, exhibiting a remarkable nanoconfinement effect. However, once the surface region of the thin film was crystallized, or frozen in terms of the segmental motion, Tg of the films recovered to that of the bulk. Concurrently, the apparent activation energy of the segmental motion in the surface-crystallized film was in good accordance with the bulk value as well. These results make it clear that the mobility in the surface region plays an essential role in the glass transition of the thin films.
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U2 - 10.1021/acs.macromol.6b02740
DO - 10.1021/acs.macromol.6b02740
M3 - Article
AN - SCOPUS:85015232517
SN - 0024-9297
VL - 50
SP - 2061
EP - 2068
JO - Macromolecules
JF - Macromolecules
IS - 5
ER -