Surface molecular motion of the monodisperse polystyrene films

Forced modulation scanning force microscopic (SFM) and lateral force microscopic (LFM) measurements of the monodisperse polystyrene (PS) films were carried out at 293 K in order to reveal surface molecular motion. Surface dynamic storage modulus, E‘, and surface loss tangent, tan δ, of the monodisperse PS films were evaluated on the basis of forced modulation SFM measurement. It was revealed that the magnitudes of surface E‘ and surface tan δ were lower and higher than those for its bulk state, respectively, in the case of the number-average molecular weight (Mn) lower than 26.6k. Based on forced modulation SFM measurements, the surface of the PS film with Mn lower than 26.6k was in a glass−rubber transition state even at 293 K, in spite of that the bulk Tg was far above 293 K. LFM measurements for the PS films revealed that the magnitude of lateral force was dependent on the scanning rate of the cantilever tip in the case of Mn lower than 40.4k. The scanning rate dependence of lateral force appeared in t...

[1]  J. Frommer,et al.  Friction measurements on phase-separated thin films with a modified atomic force microscope , 1992, Nature.

[2]  Guenter Reiter,et al.  Dewetting as a Probe of Polymer Mobility in Thin Films , 1994 .

[3]  K. A. Grosch,et al.  The relation between the friction and visco-elastic properties of rubber , 1963, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[4]  G. Reiter MOBILITY OF POLYMERS IN FILMS THINNER THAN THEIR UNPERTURBED SIZE , 1993 .

[5]  P. Hansma,et al.  Using force modulation to image surface elasticities with the atomic force microscope , 1991 .

[6]  G. Reiter Unstable thin polymer films: rupture and dewetting processes , 1993 .

[7]  A. Takahara,et al.  Imaging of Dynamic Viscoelastic Properties of a Phase-Separated Polymer Surface by Forced Oscillation Atomic Force Microscopy , 1994 .

[8]  A. Takahara,et al.  Depth Dependence of the Surface Glass Transition Temperature of a Poly(styrene-block-methyl methacrylate) Diblock Copolymer Film on the Basis of Temperature-Dependent X-ray Photoelectron Spectroscopy , 1995 .

[9]  W. Gladfelter,et al.  Probing Molecular Relaxation on Polymer Surfaces with Friction Force Microscopy , 1995 .

[10]  Benjamin M. DeKoven,et al.  Is the molecular surface of polystyrene really glassy , 1992 .

[11]  Richard A. L. Jones,et al.  Glass Transition Behavior in Ultra‐Thin Polystyrene Films , 1995 .

[12]  J. Frommer,et al.  Force Microscopy Study of Friction and Elastic Compliance of Phase-Separated Organic Thin Films , 1994 .

[13]  R. Wiesendanger Scanning Probe Microscopy and Spectroscopy: Contents , 1994 .

[14]  M. Radmacher,et al.  Imaging viscoelasticity by force modulation with the atomic force microscope. , 1993, Biophysical journal.

[15]  A. Mayes Glass Transition of Amorphous Polymer Surfaces , 1994 .

[16]  A. Takahara,et al.  Aggregation structure and surface properties of immobilized organosilane monolayers prepared by the upward drawing method , 1994 .

[17]  T. Takemura,et al.  Rolling Friction of Polymeric Material , 1967 .

[18]  Gerber,et al.  Atomic Force Microscope , 2020, Definitions.

[19]  A. Takahara,et al.  PHASE SEPARATED MORPHOLOGY OF AN IMMOBILIZED ORGANOSILANE MONOLAYER STUDIED BY A SCANNING PROBE MICROSCOPE , 1995 .

[20]  A. Takahara,et al.  Ultrathinning-Induced Surface Phase Separation of Polystyrene/Poly(vinyl methyl ether) Blend Film , 1995 .

[21]  Hertz On the Contact of Elastic Solids , 1882 .