Exchange Scattering in a Three Body Problem

Cover Exchange Scattering in a Three Body Problem
Exchange Scattering in a Three Body Problem
Harry E Moses
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Rj^^. \.^^.^^) (30) . P, (i^, X2!E, G, >', c)dT.^dx2, p, "being the eigenf unction of H . Using the orthogonality relations (l8), (12) for and h ^nd the eynression (2?) for \x, we see that (29) is equivalent to ^(x^Ill. E^. A^. P^lFt. E') = -00 _ (31) / J r(F, E«, v, pilE. E^, a^, e^)%(x2lE-E'. V)dVdE.
We shall calculate r in terms of \}r as given in the H — representation.
- 11 - Denoting v In the F hy u(F, G, V, € I^. E, a, P ), where O & ^ cl we have, on usln^ (30), (2?) and (25) together wi
...th orthogone-lity relations for and X '• r(F. G. V,

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