By J. (Ed.) Cerny
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Additional info for Nuclear Spectroscopy and Reactions, Part A
Methods 11, 4 9 . Rose, P. , and Galejs, A. ( 1 9 6 7 ) . Progr. Nucl. Tech. Instrum. 2, 3. Rose, P. , Bastide, R. , Wittkower, A. , Webb, D. , Goldie, C. H.. and Shaw, J. ( 1 9 6 0 ) . Rev. Sci. Instrum. 3 1 , 1052. Shotter, A. , and Fisher, P. S. ( 1 9 7 0 ) . Nucl Instrum. Methods 8 8 , 2 3 3 . Stenning, P. , and Trowbridge, C. W. ( 1 9 6 8 ) . Rutherford Lab. Rep. R U / R L - 1 . Takacs. J. ( 1 9 7 1 ) . Stabilization and Control of Electrostatic Generators. Dissertation, Univ. of Surrey. Taylor, I.
D. ELECTRIC FORCES We n o w consider the effect of acceleration b y t h e electrostatic field at t h e dee g a p . In t h e same w a y t h a t we solved t h e e q u a t i o n s of m o t i o n for t h e axial and radial b e t a t r o n oscillations, we can write d o w n a n d integrate the e q u a t i o n of m o t i o n of a particle w h o s e m o m e n t u m ρ s u d d e n l y b e c o m e s ρ + dp. T h e result is t h a t the particle, as might be e x p e c t e d , begins t o oscillate a r o u n d its new equilibrium orbit w i t h an a m p l i t u d e a given b y T _ * A r Q ΤΛ dp Λ ~ (16) Again, the oscillation is stable provided t h a t η is less t h a n u n i t y .
Gobbett, R. , and Stroud, P. T. ( 1 9 6 5 ) . IEEE Trans. Nucl. Sci. N S 1 2 , 246. , and Henshall, J. B. ( 1 9 5 9 ) . / . Appl Phys. 3 0 , 7 0 8 . , and Levin, J. S. ( 1 9 5 8 ) . Phys. Rev. 1 0 3 , 3 4 3 . Dawton, R. Η. V. M. ( 1 9 6 9 ) . Nucl Instrum. Methods 6 7 , 3 4 1 . Donnally, B. , and Thoeming, G. ( 1 9 6 7 ) . Phys. Rev. 159, 87. Elkind, Μ. M. ( 1 9 5 3 ) . Rev. Sci. Instrum. 2 4 , 129. Eve, A. S. ( 1 9 3 9 ) . "Rutherford," p. 338. Cambridge Univ. Press, London and N e w York. , and Hortig, G.
Nuclear Spectroscopy and Reactions, Part A by J. (Ed.) Cerny