THEORY OF BINARY BOSON SOLUTIONS. Page: 14 of 30
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can be carried out for Eqs. (12)-(14), solving for ui (r) and the
adjusted u (43) (r) and u (44)(r). Equations (12)-(14) can be put in a
9) ((, r r - 1 .,N ) (4 ,3 )
N g(3- ( )
u, (4,3)(r )
-V,(4,3) (r )
3 T(r N
- u'(r12 04 g (4)r12) +
where Q(r12) has been defined in Eqs. (22)-(24), and S(r) and T(r) are
(-1) sn(r12) ,
s (r12 4 (4,3 (1,2,N)
R(4,4,4) 1 J
Sn (12) m 4 (4,4) (1 2,3)
n-1(r13)cos(r12'13)dr3, n > 0,
T(r1 ) = -W) t (r1N) , (35
t (r1N) 0 Jg(4,3,3)(1,N-1,)u(3,3) (rN,)cos(rIN'jN-1,NdrN-'
tfl(r1) -p44 (r ,r, e)lN rd
t (3N ) P4 J g(4,3) ( (r 2N)cos(r N'r)dr2. (37
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Massey, W.E. & Tan, H. THEORY OF BINARY BOSON SOLUTIONS., report, October 31, 1970; United States. (https://digital.library.unt.edu/ark:/67531/metadc1032575/m1/14/: accessed April 19, 2019), University of North Texas Libraries, Digital Library, https://digital.library.unt.edu; crediting UNT Libraries Government Documents Department.