A Corpuscular Quantum Theory of the Scattering of Polarized X-rays

1924 ◽  
Vol 23 (3) ◽  
pp. 313-317 ◽  
Author(s):  
G. E. M. Jauncey
Keyword(s):  
1984 ◽  
Vol 85 (2) ◽  
pp. 335-348 ◽  
Author(s):  
T. Ohkawa ◽  
H. Hashimoto
Keyword(s):  

1923 ◽  
Vol 21 (5) ◽  
pp. 483-502 ◽  
Author(s):  
Arthur H. Compton
Keyword(s):  
X Rays ◽  

Nature ◽  
1924 ◽  
Vol 113 (2832) ◽  
pp. 196-196 ◽  
Author(s):  
G. E. M. JAUNCEY
Keyword(s):  

Of the various possible methods of approaching present day problems of electro­magnetic radiation—particularly the problem of reconciling with the older electro­magnetic theory those experimental facts which have led to the formulation of the Quantum Theory—the most profitable is probably to be found in the study of the phenomena of Röntgen radiation. Primarily this is due not to the accuracy which may be attained in measurements upon radiation of this type, though this is an important factor, but to the fundamental nature of the phenomena themselves. The result of this is shown both in the simplicity and in the generality of the laws observed.


It is shown that the quantum theory of X -ray reflexion and scattering in crystals developed in Part I is in full accord with the experimental facts. The theory succeeds in giving a quantitative explanation of the experimental facts concerning these phenomena as observed with diamond, viz. (1) the specular character of the quantum reflexion from the (111) planes, (2) the geometric law of such reflexion and especially the fact that, in general, the reflexion falls outside the plane of incidence, (3) the subsidiary features accompanying the reflexion, viz. faint elliptic spots and elongated streamers noticed in certain special cases, (4) the absolute intensity of the reflexion which is an appreciable fraction of the intensity of the classical reflexion, (5) the failure of the (110) planes to exhibit similar reflexions, (6) the persistence of the reflexions by the (111) planes with undiminished intensity at liquid air temperature and the relatively small increase of intensity at high temperatures, and (7) the appearance of a diffuse scattering having an undiminished intensity at low temperatures. The differences between diamond and other crystals in respect of these X -ray phenomena are explained by taking into consideration the differences in the frequency and character of their lattice vibrations in the infra-red region as revealed by the spectroscope.


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