THEORY OF BINARY BOSON SOLUTIONS. Page: 16 of 30
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describes a deformation of the liquid medium. As we shall see in the next
section, F'2 is directly related to the long wavelength limit of the effec-
tive interaction between He3 quasiparticles in a realistic He -Hey solution.
Some of the details left out of this section can be found in
IV. Numerical Results
Numerical computations following the above prescription have
been carried out for a 6% solution at an appropriate equilibrium density,
p4 - 0.218 13. In the two body potential we used the de Boer-Michels
parsmeters, r 10.220K, 6 - 2.556A.
The explicit form for the family of pair distribution functions
is taken to be
(a (r) M $ (r) + 6g
9 (r) - (C+1)exp[-(t) ] - C exp[-(l+I) ) ,
8 p (r) - A((d)6exp[-(1+y)( )1 f(A exp[-(l+q)($)3 (
where C, d, A, y and q are variational parameters, and z and a are deter-
mined by the normalization conditions, Eq. (8). This form has beea. found
in our previous work to be flexible and satisfactory for pure helium
The parameters for g (r) were determined in reference 6.
The optimum values of the parameters for g(3 (r) and g (r) are
given in Table 1. Since at low mass-3 concentrations a simpler form
should suffice for g * (r), we have chosen A to be zero in g * (r)
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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/m1/16/: accessed April 26, 2019), University of North Texas Libraries, Digital Library, https://digital.library.unt.edu; crediting UNT Libraries Government Documents Department.