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Volumn 42, Issue 3, 1998, Pages 271-276

Controlling the dynamics of soft spheres: From polymeric to colloidal behavior

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EID: 0032073743     PISSN: 02955075     EISSN: None     Source Type: Journal    
DOI: 10.1209/epl/i1998-00241-3     Document Type: Article
Times cited : (56)

References (26)
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    • DAOUD M. and COTTON J. B., J. Phys. (Paris), 43 (1982) 831; WITTEN T., PINCUS P. A. and GATES M. E., Europhys. Lett., 2 (1986) 137; GREST G. S., HUANG J., FETTERS L. J. and RICHTER D., Adv. Chem. Phys., XCIV (1996) 67.
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    • Witten, T.1    Pincus, P.A.2    Gates, M.E.3
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    • DAOUD M. and COTTON J. B., J. Phys. (Paris), 43 (1982) 831; WITTEN T., PINCUS P. A. and GATES M. E., Europhys. Lett., 2 (1986) 137; GREST G. S., HUANG J., FETTERS L. J. and RICHTER D., Adv. Chem. Phys., XCIV (1996) 67.
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    • note
    • 1/(3ν - 1) beyond which phase sepatation is predicted.
  • 17
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    • note
    • Note the difference between the overlap volume fraction of polymers (typically here about 0.1) and close-packing volume fraction of colloids (typically about 0.45), reflecting the fractal dimension of the former versus the 3D compact structure of the latter.
  • 19
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    • The process intensity is computed from the total average scattering intensity I(q) and the amplitude (≤ 1) of the particular decay
    • The process intensity is computed from the total average scattering intensity I(q) and the amplitude (≤ 1) of the particular decay.
  • 20
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    • The variation of intensity with c exhibits a maximum at c*
    • The variation of intensity with c exhibits a maximum at c*.
  • 21
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  • 23


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.