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Volumn 107, Issue 1, 2003, Pages 96-101

Spontaneous correlation of crystallographic orientations in crystallite aggregation: Physical origin and its influence on pattern formation

Author keywords

[No Author keywords available]

Indexed keywords

AGGLOMERATION; ANISOTROPY; ATOMIC FORCE MICROSCOPY; CORRELATION THEORY; CRYSTAL GROWTH; CRYSTAL ORIENTATION; FRACTALS; NUCLEATION; PATTERN MATCHING; SURFACE TENSION; X RAY DIFFRACTION ANALYSIS;

EID: 0037426927     PISSN: 10895647     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp026615v     Document Type: Article
Times cited : (20)

References (33)
  • 6
    • 0002489522 scopus 로고    scopus 로고
    • and references therein
    • Politi, P.; et al. Phys. Rep. 2000, 324, 271 and references therein.
    • (2000) Phys. Rep. , vol.324 , pp. 271
    • Politi, P.1
  • 8
    • 0012633145 scopus 로고    scopus 로고
    • Ph. D thesis, McGill University, Montreal, 1998
    • Müller, J. Ph. D thesis, McGill University, Montreal, 1998.
    • Müller, J.1
  • 22
    • 0012739569 scopus 로고    scopus 로고
    • note
    • Before carrying out computer simulation, we first determine the coordinates of the center of each elongated diffraction spot in the experimental diffraction pattern. The orientation of a crystallite is characterized by Euler angles θ, φ, and ψ. In calculation the wavelength of X-ray is set between 0.7 and 2.2 Å. θ, φ and ψ are changed with a step of 2 mRod. This step size corresponds to a linear separation of about 50 microns in the diffraction spectrum in our experiment. At each step the diffraction pattern is calculated and compared with the experimental data. Once a bestfit combination of θ, φ, and ψ is found, we continue to determine the axis of the orientation rotation and the degree that the crystallite has been rotated in a similar way. If the computed direction of the spot elongation is in agreement with the experimental observation, we conclude that the correct axis of rotation has been found. It is noteworthy that the noise-to-signal ratio in our experiments is not high, so many high-indexed diffraction spots cannot be identified. As a matter of fact, the analysis of the diffraction spots on the image plate shows that the diffraction coming from hkl > 2 is so weak that those spots are virtually not seen. For this reason we only consider hkl ≤ 2in the computer calculation.
  • 23
    • 0012738733 scopus 로고    scopus 로고
    • note
    • →, respectively.
  • 25
    • 0003905979 scopus 로고
    • Hurle, D. T. J., Ed.; Elsevier: New York
    • Bennema, P. In Handbook of Crystal Growth; Hurle, D. T. J., Ed.; Elsevier: New York, 1993; Vol. 1a.
    • (1993) Handbook of Crystal Growth , vol.1 A
    • Bennema, P.1
  • 27
    • 0012678692 scopus 로고    scopus 로고
    • When the supersaturation is higher than 0.2, it has been found 〈111〉 is the fast growth direction. See ref 26 for details
    • When the supersaturation is higher than 0.2, it has been found 〈111〉 is the fast growth direction. See ref 26 for details.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.