Comparison of molecular motion between linear polystyrenes and cyclic polystyrenes with same molecular weight

Daisuke Kawaguchi; Atsushi Takano; Yushu Matsushita; Naoya Torikai; Keiji Tanaka; Toshihiko Nagamura; Robert Dalgliesh; Sean Langridge

Comparison of molecular motion between linear polystyrenes and cyclic polystyrenes with same molecular weight

Daisuke Kawaguchi, Atsushi Takano, Yushu Matsushita, Naoya Torikai, Keiji Tanaka, Toshihiko Nagamura, Robert Dalgliesh, Sean Langridge

Research output: Contribution to conference › Paper › peer-review

Abstract

Time evolution of interfacial thicknesses between a cyclic polystyrene (c-hPS) / its deuterated counterpart (c-dPS) and a linear polystyrene (1-hPS) / its deuterated counterpart (1-dPS) bilayer films was investigated by dynamic secondary ion mass spectrometry (DSIMS) and neutron reflectivity (NR). The interfacial thickness of (c-hPS/c-dPS) film was significantly larger than that of (1-hPS/1-dPS) film at any given annealing time, indicating that the diffusion constant of c-PS is constantly larger than that of 1-PS. It might be explained that weaker topological constraint comes from the entanglement for the c-PS than for the 1-PS.

Original language	English
Pages	3131-3132
Number of pages	2
Publication status	Published - 2006
Event	55th Society of Polymer Science Japan Symposium on Macromolecules - Toyama, Japan Duration: Sept 20 2006 → Sept 22 2006

Other

Other	55th Society of Polymer Science Japan Symposium on Macromolecules
Country/Territory	Japan
City	Toyama
Period	9/20/06 → 9/22/06

All Science Journal Classification (ASJC) codes

Engineering(all)

Cite this

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title = "Comparison of molecular motion between linear polystyrenes and cyclic polystyrenes with same molecular weight",

abstract = "Time evolution of interfacial thicknesses between a cyclic polystyrene (c-hPS) / its deuterated counterpart (c-dPS) and a linear polystyrene (1-hPS) / its deuterated counterpart (1-dPS) bilayer films was investigated by dynamic secondary ion mass spectrometry (DSIMS) and neutron reflectivity (NR). The interfacial thickness of (c-hPS/c-dPS) film was significantly larger than that of (1-hPS/1-dPS) film at any given annealing time, indicating that the diffusion constant of c-PS is constantly larger than that of 1-PS. It might be explained that weaker topological constraint comes from the entanglement for the c-PS than for the 1-PS.",

author = "Daisuke Kawaguchi and Atsushi Takano and Yushu Matsushita and Naoya Torikai and Keiji Tanaka and Toshihiko Nagamura and Robert Dalgliesh and Sean Langridge",

year = "2006",

language = "English",

pages = "3131--3132",

note = "55th Society of Polymer Science Japan Symposium on Macromolecules ; Conference date: 20-09-2006 Through 22-09-2006",

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TY - CONF

T1 - Comparison of molecular motion between linear polystyrenes and cyclic polystyrenes with same molecular weight

AU - Kawaguchi, Daisuke

AU - Takano, Atsushi

AU - Matsushita, Yushu

AU - Torikai, Naoya

AU - Tanaka, Keiji

AU - Nagamura, Toshihiko

AU - Dalgliesh, Robert

AU - Langridge, Sean

PY - 2006

Y1 - 2006

N2 - Time evolution of interfacial thicknesses between a cyclic polystyrene (c-hPS) / its deuterated counterpart (c-dPS) and a linear polystyrene (1-hPS) / its deuterated counterpart (1-dPS) bilayer films was investigated by dynamic secondary ion mass spectrometry (DSIMS) and neutron reflectivity (NR). The interfacial thickness of (c-hPS/c-dPS) film was significantly larger than that of (1-hPS/1-dPS) film at any given annealing time, indicating that the diffusion constant of c-PS is constantly larger than that of 1-PS. It might be explained that weaker topological constraint comes from the entanglement for the c-PS than for the 1-PS.

AB - Time evolution of interfacial thicknesses between a cyclic polystyrene (c-hPS) / its deuterated counterpart (c-dPS) and a linear polystyrene (1-hPS) / its deuterated counterpart (1-dPS) bilayer films was investigated by dynamic secondary ion mass spectrometry (DSIMS) and neutron reflectivity (NR). The interfacial thickness of (c-hPS/c-dPS) film was significantly larger than that of (1-hPS/1-dPS) film at any given annealing time, indicating that the diffusion constant of c-PS is constantly larger than that of 1-PS. It might be explained that weaker topological constraint comes from the entanglement for the c-PS than for the 1-PS.

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M3 - Paper

AN - SCOPUS:33846165430

SP - 3131

EP - 3132

T2 - 55th Society of Polymer Science Japan Symposium on Macromolecules

Y2 - 20 September 2006 through 22 September 2006

ER -

Comparison of molecular motion between linear polystyrenes and cyclic polystyrenes with same molecular weight

Abstract

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All Science Journal Classification (ASJC) codes

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