The Stability of a Span Classsearchtermclassspan of Bifurcated Magnetoh

Cover The Stability of a Span Classsearchtermclassspan of Bifurcated Magnetoh
The Stability of a Span Classsearchtermclassspan of Bifurcated Magnetoh
Jay Kappraff
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(T^°^ + ?^^h)^ . (94) We again find it useful to decompose 6W into 01 10 11 48 Once again 5W^^^^ Is Identical with the preblfurcated results, and referring to (53), 6W^^^^ = 2uHc^e^( i c^sl p) . (95) 11 ^ ^'" From (80) and (9 4), we find after a long computation, (1)^ + 6W(1)^ = 2. H, 2e2(_ li^V^ c^aS, _, ] . (96) 6W 01 10 (1)V.
We decompose 6W^^ Into three terms: 01 10 11 where 6W^1^^ = f r|H|$^°^n. V$^l)dedz 01 J '^^ 6W^1^^ = f rlH|$^l^n. V$^°^dedz 10 J '^ 6W^1)^ = f rlHI^^l^n. V^^l^dSdz 11 w
...here $ Is given by (84), while $ is the scalar potential that results from Q and the boundary condition (26).
From (48 ), Q^-"-^ = 2icec^6„ „r exp [21(6 + z)](ir - 0) + 2iYec^62 _2i^ exp [21(6 + z)](ir + 6) 49 Thus, 2, -2 + exp [2i(-6 + z)] xp [21(6+z)] 1 :97) i From (85) and (97), solving (26 ) order by order, ^^^ = Cec^62^_2

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