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The values of 3/ G, h a n d Q were used i n going from one ease t o t h e next were estimated by use of equations (27a and b). - h. 73 x 10-27cm2 p l u s and minus two and one-half percent. The l a s t iterates u(x) and w(x) f o r t h e prev%ously computed case w i t h c l o s e s t y v a l u e were used as t h e f i r s t approximation t o t h e wave functions. 1 pereent of i t s f i n a l value. However, Q was q u i t e s e n s i t i v e t o t h e wave f u n c t i o n s and after two i t e r a t i o n s o f t e n had not completely s e t t l e d down, I n t h e few cases where two i t e r a t i o n s and the use of equations (36) and (39) were i n s u f f i c i e n t t o y i e l d t h e d e s i r e d accuracy i n L a n d Q, wave f u n c t i o n s u,(x) and w ( x ) were computed by use o f the followfng e x t r a p o l a t i o n 3 formulas obtained from equation (26) I -a- and Then u,(x) and w3(x) were introduced i n t o equations (32a and b) and t h e iterates u4(x) and w ( x ) obtained.

8550 4. 1509 I . 309? 1735 . 4588 . 3000 X . 2392 17'. 376 5212 . 072. 9417 . 368 . 368 . 0978 X ~ . 1185 TABLE S Grs u-6. 1900 i . 9092 7. a645 7. 2400 ~ ~ 2 . 4118 4 I- ,. 1550 X J i . 9974 I. 4893 8 .? 9251. 7300 t . 4096 7. 2400 ,. T. 65 65 ,. 2400 * 0245 ,. Ob0 61 61 ,. 33 T . 7107 095. O59 .

0978 X ~ . 1185 TABLE S Grs u-6. 1900 i . 9092 7. a645 7. 2400 ~ ~ 2 . 4118 4 I- ,. 1550 X J i . 9974 I. 4893 8 .? 9251. 7300 t . 4096 7. 2400 ,. T. 65 65 ,. 2400 * 0245 ,. Ob0 61 61 ,. 33 T . 7107 095. O59 .

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Effect of Tensor Range in Nuclear Two-Body Problems


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