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Volumn 36, Issue 4, 2003, Pages 1199-1208

Ultrathin films of poly(ethylene oxides) on oxidized silicon. 2. In situ study of crystallization and melting by hot stage AFM

Author keywords

[No Author keywords available]

Indexed keywords

ATOMIC FORCE MICROSCOPY; CRYSTAL GROWTH; CRYSTALLIZATION; GLASS TRANSITION; ISOTHERMS; MELTING; OXIDATION; SILICON; THERMAL EFFECTS; ULTRATHIN FILMS;

EID: 0037465026     PISSN: 00249297     EISSN: None     Source Type: Journal    
DOI: 10.1021/ma020686a     Document Type: Article
Times cited : (186)

References (84)
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    • See ref 28.
    • (b) See ref 28.
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    • In the course of writing these manuscripts a similar study has been published by Dalnoki-Veress et al. which describes the reduction of crystallization rates for PEO thin films on silicon and gold substrates as studied by quartz crystal microbalance and video optical microscopy (Dalnoki-Veress, N.; Forrest, J. A.; Massa, M. V.; Pratt, A.; Williams, A. J. Polym. Sci., Part B: Polym. Phys. 2001, 39, 2615). The complementary results reported by these authors are in good agreement with our data.
    • (2001) J. Polym. Sci., Part B: Polym. Phys. , vol.39 , pp. 2615
    • Dalnoki-Veress, N.1    Forrest, J.A.2    Massa, M.V.3    Pratt, A.4    Williams, A.5
  • 50
    • 0031544451 scopus 로고    scopus 로고
    • Studies on polymer crystallization close to room temperature (without active control of the specimen temperature) have been reported: e.g. McMaster, T. J.; Hobbs, J. K.; Barham, P. J. Miles, M. J. Probe Microsc. 1997, 1, 43.
    • (1997) Probe Microsc. , vol.1 , pp. 43
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  • 53
    • 0032205265 scopus 로고    scopus 로고
    • Recently, Marand et al. have shown that the established linear Hoffman-Weeks extrapolation leads to a significant underestimation of the equilibrium melting temperature (Marand, H.; Xu, J.; Srinivas, S. Macromolecules 1998, 31, 8219). In this work we have utilized the linear extrapolation, and hence our result is likely an underestimate. Taking the limited number of available data points into account, we were unable to perform the correct nonlinear extrapolation.
    • (1998) Macromolecules , vol.31 , pp. 8219
    • Marand, H.1    Xu, J.2    Srinivas, S.3
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    • Academic Press: New York
    • For discussion of various aspects of polymer crystallization see e.g.: (a) Wunderlich, B. Macromolecular Physics; Academic Press: New York, 1973, 1976, 1980; Vols. 1, 2, 3.
    • (1973) Macromolecular Physics , vol.1-3
    • Wunderlich, B.1
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    • Kluwer Academic Publishers: Dordrecht
    • (e) Gedde, U. Polymer Physics, 1st ed.; Kluwer Academic Publishers: Dordrecht, 1995.
    • (1995) Polymer Physics, 1st Ed.
    • Gedde, U.1
  • 59
    • 0003903898 scopus 로고
    • NATO ASI Series; Kluwer Academic Publishers: Dordrecht
    • (f) Crystallization of Polymers; Dosiere, M., Ed.; NATO ASI Series; Kluwer Academic Publishers: Dordrecht, 1993.
    • (1993) Crystallization of Polymers
    • Dosiere, M.1
  • 67
    • 0003716582 scopus 로고
    • Wiley-Interscience: New York, Chapter 3
    • Geil, P. H. Polymer Single Crystals; Wiley-Interscience: New York, 1963; Chapter 3.
    • (1963) Polymer Single Crystals
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  • 70
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    • Doremus, R. H., Roberts, B. W., Turnbull, D., Eds.; Wiley: New York
    • Keller, A. In Growth and Perfection of Crystals; Doremus, R. H., Roberts, B. W., Turnbull, D., Eds.; Wiley: New York, 1958; p 499.
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    • Keller, A.1
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    • Reference 43c.
    • (c) Reference 43c.
  • 74
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    • note
    • For the specific case of thin films of PEO, the AFM data acquisition is limited to lamellar growth rates of ca. 0.5-1.0 μm/s and slower. This estimate is based on the growth of a lamellar crystal over the distance of a typical scan size of 20 μm within the time elapsed to capture six subsequent images using the following parameters: resolution = 128 pixels/line, 16 lines scanned, scan rate = 2.5-5.0 Hz.
  • 79
    • 0012271866 scopus 로고    scopus 로고
    • note
    • 0/kδH. Regime I growth (j = 2) refers to the situation where the secondary nucleation step controls the linear growth rate and regime II growth (j = 1) refers to the multiple nucleation case, while regime III growth (j = 2) characterizes prolific nucleation; see refs 44 and 43e, p 178). On the basis of a comparison of the temperature and molar mass range investigated, we tentatively assign our data to regime III growth in accordance with ref 55.
  • 80
    • 36549100911 scopus 로고
    • Simulation work by various methods suggested disturbed single chain properties for polymer molecules near a wall in the melt. (a) Ten Brinke, G.; Ausserre, D.; Hadziioannou, G. J. Chem. Phys. 1988, 89, 4374.
    • (1988) J. Chem. Phys. , vol.89 , pp. 4374
    • Ten Brinke, G.1    Ausserre, D.2    Hadziioannou, G.3
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    • (c) Bitsanis, I.; Hadziioannou, G. J. Chem. Phys. 1990, 92, 3827.
    • (1990) J. Chem. Phys. , vol.92 , pp. 3827


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