6.16
The deuteron is a nucleus of heavy hydrogen consisting of ne proton and one neutron.As a simple model for this nucleos consider a single particle of mass m moving in a fixed spehreical -symmetric potencial V(r) defined by V(r)=-Vo for rro .This is called a spherical square well potential.Asssume that the particle is in a bound state with l=0
a) Fin the general solutions R(r) to the radical Schoringer euatio for rro.Use the fact that the wave function must be finite at 0 and ∞ to simpfy the solution as much as possible.(You don’t have to normalieze the solutions)
THIS PICTURE IS THE ANSWER ,BUT I DON’T UNDERSTAND WHY B1=0 AND A2=0. Could you please DRAW THE WAVE and explain it !! My book said r=0 and u(0)= 0 so B1 = 0.I don’t understand why and how the wave works here. Thank you
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6.16 The deuteron is a nucleus of heavy hydrogen consisting of ne proton and one neutron.As...
Consider a particle of mass m in an infinite spherical potential well of radius a For write down the energies and corresponding eigen functions ψ--(r,0.9). (3 pt) a) ne that at t-o the wave function is given by o)-A. Find the normalization constant A function in this basis. Solve for the coeffici You may find useful the integrals in the front of the (6 pt) d) Now consider the finite potential spherical well with V(r)- ing only the radial part...
A NON stationary state A particle of mass m is in an infinite square well potential of width L, as in McIntyre's section 5.4. Suppose we have an initial state vector lv(t -0) results from Mclntrye without re-deriving them, and you may use a computer for your math as long as you include your code in your solution A(3E1) 4iE2)). You may use E. (4 pts) Use a computer to plot this probability density at 4 times: t 0, t2...