Paracrystalline lattice distortion in the near-surface region of melt-crystallized polyethylene films evaluated by synchrotron-sourced grazing-incidence X-ray diffraction
Paracrystalline lattice distortion in the near-surface region of melt-crystallized polyethylene films evaluated by synchrotron-sourced grazing-incidence X-ray diffraction
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DOI:
10.1021/ma034526q
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发表时间:
2003-07
期刊:
影响因子:
5.5
通讯作者:
Hirohiko Yakabe;S. Sasaki;O. Sakata;A. Takahara;T. Kajiyama
中科院分区:
文献类型:
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作者:
Hirohiko Yakabe;S. Sasaki;O. Sakata;A. Takahara;T. Kajiyama
Physical properties of polymeric materials such as adhesion and friction relate to molecular aggregation structure in the material’s surface. However, the surface of crystalline polymers has been studied mainly from morphological and chemical points of view. In the case of polyethylene (PE), a typical example of crystalline polymers, the surface morphology of its solid films was visualized in the lamellar scale by atomic force microscopy and transmission electron microscopy. 1-3 However, the crystal structure at the surface of PE films has not yet been clarified. Clarification of the crystal structure on the film surface is quite important for understanding the surface property from the molecular level. A grazing incidence X-ray diffraction (GIXD) using evanescent X-rays has recently been applied for evaluating chainpacking structure and chain orientation in the nearsurface region of crystalline polymers. 4-8 In this study, the dimension and distortion of the crystal lattice in the near-surface region of melt-crystallized PE films were investigated by synchrotron-sourced GIXD measurements.A high-density polyethylene (HDPE, MI) 14, Mitsui Chemicals, Inc.) was used as a sample. Films with a thickness of ca. 400 nm were prepared on the crystallographic (110) plane of silicon substrates from a 1.0 wt% p-xylene solution of HDPE by a dip-coating method under a nitrogen atmosphere. The size of silicon substrates used was 1 in. in diameter and 3 mm in thickness. The thus-prepared PE films were melted at ca. 443 K and then isothermally crystallized at Tc) 378, 383, 388, and 393 K for 24 h. The crystal structure in the near-surface region of the films was investigated by in-plane measurements of grazing-incidence wide-angle X-ray diffraction (GIXD). GIXD measurements were carried out on the films at 300 K with a six-axis diffractometer installed at a BL-13XU beamline of SPring-8 (Japan Synchrotron Radiation Research Institute, Hyogo, Japan). 9 The wavelength, λ, of monochromatized incident X-rays used in this study was 0.1285 or 0.1280 nm. The beam size at incident slits was