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Volumn 33, Issue 3, 2000, Pages 968-977

Order-order phase transition between spherical and cylindrical microdomain structures of block copolymer. I. Mechanism of the transition

Author keywords

[No Author keywords available]

Indexed keywords

CRYSTAL LATTICES; CRYSTAL MICROSTRUCTURE; CRYSTAL ORIENTATION; CRYSTALLOGRAPHY; GRAIN SIZE AND SHAPE; MOLECULAR WEIGHT; ORDER DISORDER TRANSITIONS; POLYISOPRENES; POLYSTYRENES; X RAY SCATTERING;

EID: 0034620342     PISSN: 00249297     EISSN: None     Source Type: Journal    
DOI: 10.1021/ma991470k     Document Type: Article
Times cited : (107)

References (39)
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    • (b)Hashimoto, T. In Thermoplastic Elastomers; Legge, N. R., Holden, G., Schroeder, H. E., Eds.; Hanser, Munich, Germany, 1987.
    • (1987) Thermoplastic Elastomers
    • Hashimoto, T.1
  • 7
    • 0027683885 scopus 로고
    • Sakurai, S.; Kawada, H.; Hashimoto, T.; Fetters, L. J. Proc. Jpn. Acad. 1993, 69 (Ser. B), 13; Macromolecules 1993, 26, 5796.
    • (1993) Macromolecules , vol.26 , pp. 5796
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    • Porod, G. Kolloid, Z. Z. Polym. 1951, 124, 83; 1952, 125, 51; 1952, 125, 108.
    • (1952) Z. Polym. , vol.125 , pp. 51
  • 27
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    • Porod, G. Kolloid, Z. Z. Polym. 1951, 124, 83; 1952, 125, 51; 1952, 125, 108.
    • (1952) Z. Polym. , vol.125 , pp. 108
  • 28
    • 0343072983 scopus 로고
    • Mayer, M. G., Ed.; John Wiley and Sons Publishers: New York
    • See, for example: Guinier, A.; Fournet, G. In Small-Angle Scattering of X-rays; Mayer, M. G., Ed.; John Wiley and Sons Publishers: New York, 1955; pp 111-120. Actually, the size of the incident beam is finite in our SAXS facility, however, the smearing effect was nearly equal to that for the infinite slit height. About the details, see, for example: Hashimoto, T.; Fujimura, M.; Kawai, H. Macromolecules 1980, 13, 1660.
    • (1955) Small-Angle Scattering of X-rays , pp. 111-120
    • Guinier, A.1    Fournet, G.2
  • 29
    • 0000524598 scopus 로고
    • See, for example: Guinier, A.; Fournet, G. In Small-Angle Scattering of X-rays; Mayer, M. G., Ed.; John Wiley and Sons Publishers: New York, 1955; pp 111-120. Actually, the size of the incident beam is finite in our SAXS facility, however, the smearing effect was nearly equal to that for the infinite slit height. About the details, see, for example: Hashimoto, T.; Fujimura, M.; Kawai, H. Macromolecules 1980, 13, 1660.
    • (1980) Macromolecules , vol.13 , pp. 1660
    • Hashimoto, T.1    Fujimura, M.2    Kawai, H.3
  • 31
    • 0343072981 scopus 로고    scopus 로고
    • note
    • Strictly speaking, relative positions of higher order scattering maximum in a SAXS profile indicate only the lattice type but not the shape of microdomains. To determine the shape, the particle scattering due to the intra-microdomain interference (form factor) should be taken into consideration, though, in our experiment the form factor was not clearly observed. For PS-PI diblock copolymer it is well-known that the spherical domain structure (bcc-sphere or spheres in a face-centered cubic lattice (fcc-sphere)) appears for the A-B block copolymer with/ f < 0.17 (or f > 0.76), and the cylindrical structure occurs over the range of 0.17 < f < 0.33 (or 0.67 < f < 0.76). (see ref 2-4). In our case of f = 0.18, the block copolymer seems to have spherical or cylindrical microdomain structure. These three structures are easy to be distinguished by only the relative positions of higher order scattering maximum (1, √2, √3, √4, √5, √6, etc for bcc-sphere; 1, √4/3, √8/3, √11/3, √12/3, etc for fcc-sphere; 1, √3, √4, √7, √9, √12, √13, etc for hex-cylinder).
  • 32
    • 3643121692 scopus 로고    scopus 로고
    • Schwab, M.; Stühn, B. Phys. Rev. Lett. 1996, 76, 924. In this work, however, the state with LDS was defined as the disordered state. We should note, however, that this state is different from the disordered state in lamella-or cylinder-forming block copolymers, simply because the block copolymer in LDS is microphase-separated and the microdomains having a well-defined interface are still static objects, persisting as a structural entity at any time instances in the time scale of our SAXS experiments: they are not dynamical objects which are generated and relaxed with a certain relaxation time. Note also that the microphase-separated state has less entropy than the disordered state free from the microphase-separated structure.
    • (1996) Phys. Rev. Lett. , vol.76 , pp. 924
    • Schwab, M.1    Stühn, B.2
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    • note
    • 1/2.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.