Onset of tethered chain overcrowding

被引:135
作者
Chen, WY
Zheng, JX
Cheng, SZD [1 ]
Li, CY
Huang, P
Zhu, L
Xiong, HM
Ge, Q
Guo, Y
Quirk, RP
Lotz, B
Deng, LF
Wu, C
Thomas, EL
机构
[1] Univ Akron, Maurice Morton Inst, Akron, OH 44325 USA
[2] Univ Akron, Dept Polymer Sci, Akron, OH 44325 USA
[3] Drexel Univ, Dept Mat Sci & Engn, Philadelphia, PA 19104 USA
[4] Univ Connecticut, Inst Mat Sci, Polymer Program, Storrs, CT 06269 USA
[5] Univ Connecticut, Dept Chem Engn, Storrs, CT 06269 USA
[6] Inst Charles Sadron, F-67083 Strasbourg, France
[7] Chinese Univ Hong Kong, Dept Phys, Sha Tin, Hong Kong, Peoples R China
[8] Chinese Univ Hong Kong, Dept Chem, Sha Tin, Hong Kong, Peoples R China
[9] MIT, Dept Mat Sci & Engn, Cambridge, MA 02139 USA
基金
美国国家科学基金会;
关键词
D O I
10.1103/PhysRevLett.93.028301
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We proposed an approach to precisely control the density of tethered chains on solid substrates using PEO-b-PS and PLLA-b-PS. As the crystallization temperature T-x increased, the PEO or PLLA lamellar crystal thickness d(L) increased as well as the reduced tethering density (σ) over tilde of the PS chains. The onset of tethered PS chains overcrowding in solution occurs at (σ) over tilde*similar to3.7-3.8 as evidenced by an abrupt change in the slope between (d(L))(-1) and T-x. This results from the extra surface free energy created by the tethered chain that starts to affect the growth barrier of the crystalline blocks.
引用
收藏
页码:028301 / 1
页数:4
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