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In view of the smaller new val . of the meson lifetime ( cf. preceding abstract ) , theoretical vals . for the intensity of the soft component due to meson decay are compared with experimental data . N. M. B. Mean life of slow mesotrons ...
In view of the smaller new val . of the meson lifetime ( cf. preceding abstract ) , theoretical vals . for the intensity of the soft component due to meson decay are compared with experimental data . N. M. B. Mean life of slow mesotrons ...
Trang 325
All photographs showed a shift > 0 for the max . intensity of the non - Laue spot from the position of the corresponding Bragg spectrum line . Results differ from those of Raman ( cf. A. , 1940 , I , 348 , 431 ) and from Zachariasen's ...
All photographs showed a shift > 0 for the max . intensity of the non - Laue spot from the position of the corresponding Bragg spectrum line . Results differ from those of Raman ( cf. A. , 1940 , I , 348 , 431 ) and from Zachariasen's ...
Trang 439
I. Spectral intensity distribution . R. C. Garth and G. E. Moore ( Physical Rev. , 1941 , [ ii ] , 60 , 208—215 , 216–224 ) .- I . The intensities of the stronger lines in the subordinate series of the afterglow spectrum were measured ...
I. Spectral intensity distribution . R. C. Garth and G. E. Moore ( Physical Rev. , 1941 , [ ii ] , 60 , 208—215 , 216–224 ) .- I . The intensities of the stronger lines in the subordinate series of the afterglow spectrum were measured ...
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