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1.
H. Y.
Ku
and
F. G.
Ullman
,
J. Appl. Phys.
35
,
265
(
1964
).
2.
C. A.
Mead
,
Phys. Rev. Letters
6
,
545
(
1961
).
3.
In arriving at Eqs. (13) and (14), the boundary conditions used were ν = ν1 at r = 0 and dv/dr = 0, at r = ∞, and ν = ν2 at r = 0 and dv/dr = 0 at r = ∞, respectively, as Ku and Ullman’s boundary conditions prove inconsistent.
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