ATOMIC AND NUCLEAR PHYSICS PLEASE ANSWER ALL QUESTIONS Let us consider that the two particles interact via an attractive square well potential, i.e -Uo TSR V(r)= 0 r> R, where R = 1.2 fm(4/³+A), with A1 and A2, the particles' atomic masses. For the s-wave state (= 0), the above equation has the following form Csin(Kr) T≤R to(k,r) == sin(kr +80) r> R₁ where C is a normalization constant, K² = √(k+Uo), and do the scattering phase shift. Using the continuity of the wave function and its derivative at r= R, i.e Csin(KR) = sin(kR+ 8), d dR Csin(KR) = sin(kR+60), d dR (a) show that the phase phift is given by
ATOMIC AND NUCLEAR PHYSICS PLEASE ANSWER ALL QUESTIONS Let us consider that the two particles interact via an attractive square well potential, i.e -Uo TSR V(r)= 0 r> R, where R = 1.2 fm(4/³+A), with A1 and A2, the particles' atomic masses. For the s-wave state (= 0), the above equation has the following form Csin(Kr) T≤R to(k,r) == sin(kr +80) r> R₁ where C is a normalization constant, K² = √(k+Uo), and do the scattering phase shift. Using the continuity of the wave function and its derivative at r= R, i.e Csin(KR) = sin(kR+ 8), d dR Csin(KR) = sin(kR+60), d dR (a) show that the phase phift is given by
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