Integrated Intensities of the Diffracted and Transmitted X-rays due to ideally Perfect Crystal (Laue Case)

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概要

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• The analytical expressions of the integrated reflecting power and transmitting power of X-rays for absorbing perfect crystals are obtained as follows: The diffracted wave: R_<H^y>=e^<-μ_0t>・π/2[2Σ^^∞__<n=0>J_<2n+1>(2A)+I_0(h)-1]. The transmitted wave: R_<T^y>=e^<-μ_0t>・(-2π)[Σ^^∞__<m=1>mcosmβI_m(h)]-R_<H^y>. In these formulae h=2A√<k^2+g^2> and β=tan^<-1>k/g. J_m is the first kind Bessel function of m-th order and I_m is the modified Bessel function of m-th order, and the other notations are the same as those of Zachariasen's text-book on X-ray diffraction (1944). A practical method of obtaining the numerical values of R_<H^y> and R_<T^y>, and calculated results are shown.

• 社団法人日本物理学会の論文
• 1955-01-05

著者

• Kato Norio

  Kobayasi Institute Of Physical Research

関連論文

• Anomalous Enhancement of X-ray Reflection Intensity at the Boundary of Ground and Etched Regions on Crystal Surface
• Fibrous Growth of NaClO_3 on Single Crystal
• Integrated Intensities of the Diffracted and Transmitted X-rays due to ideally Perfect Crystal (Laue Case)

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