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[SOLVED] Griffiths Quantum 2.51
This is problem 2.51 from Griffiths Introduction to Quantum Mechanics, 2nd ed. p89.
Homework Statement
Consider the potential
V(x) = -\frac{\hbar^2 a^2}{m}sech^2(a x)
where a is a positive constant, and "sech" stands for the hyperbolic secant.
a) Graph this potential.
b) Check that this potential has the ground state
\psi_0(x) = A sech(a x)
and find its energy. Normalize \psi_0, and sketch its graph.
c) Show that the function
\psi_k(x) = A\left(\frac{i k - a tanh(a x)}{i k + a}\right)e^{i k x}
(where k = \sqrt{2 m E}/\hbar as usual) solves the Schr\ddot{o}dinger equation for any (positive) energy E. Since tanh z \rightarrow -1 as z \rightarrow -\infty,
\psi_k(x) \approx A e^{i k x}, for large negative x.
This represents, then, a wave coming in from the left with no accompanying reflected wave (i.e., no term exp(-ikx)). What is the asymptotic form of \psi_k(x) at large positive x? What are R and T, for this potential? Comment: This is a famous example of a reflectionless potential - every incident particle, regardless of its energy, passes right through.
The attempt at a solution
Part a is easy, just draw the graph, intersecting the y-axis at -\frac{\hbar^2 a^2}{m}.
Part b is a little more difficult. I can show that it is a solution, but I'm not sure how to guarantee that it's the ground state. With that potential, I get that
\hat H\psi_0 = -\frac{\hbar^2 a^2}{2 m} \psi_0
If this result was the same as the minimum potential, I could say for certain that it's the ground state.
And for the normalization constant I get
A = \sqrt{\frac{a}{2}}
Part c I don't have much clue for. I tried just putting the hamiltonian into mathematica with that wave function, to see what it gives me, but it didn't give me anything that I can see looks like the RHS of the equation, any suggestions on how to go about part c would be appreciated.
This is problem 2.51 from Griffiths Introduction to Quantum Mechanics, 2nd ed. p89.
Homework Statement
Consider the potential
V(x) = -\frac{\hbar^2 a^2}{m}sech^2(a x)
where a is a positive constant, and "sech" stands for the hyperbolic secant.
a) Graph this potential.
b) Check that this potential has the ground state
\psi_0(x) = A sech(a x)
and find its energy. Normalize \psi_0, and sketch its graph.
c) Show that the function
\psi_k(x) = A\left(\frac{i k - a tanh(a x)}{i k + a}\right)e^{i k x}
(where k = \sqrt{2 m E}/\hbar as usual) solves the Schr\ddot{o}dinger equation for any (positive) energy E. Since tanh z \rightarrow -1 as z \rightarrow -\infty,
\psi_k(x) \approx A e^{i k x}, for large negative x.
This represents, then, a wave coming in from the left with no accompanying reflected wave (i.e., no term exp(-ikx)). What is the asymptotic form of \psi_k(x) at large positive x? What are R and T, for this potential? Comment: This is a famous example of a reflectionless potential - every incident particle, regardless of its energy, passes right through.
The attempt at a solution
Part a is easy, just draw the graph, intersecting the y-axis at -\frac{\hbar^2 a^2}{m}.
Part b is a little more difficult. I can show that it is a solution, but I'm not sure how to guarantee that it's the ground state. With that potential, I get that
\hat H\psi_0 = -\frac{\hbar^2 a^2}{2 m} \psi_0
If this result was the same as the minimum potential, I could say for certain that it's the ground state.
And for the normalization constant I get
A = \sqrt{\frac{a}{2}}
Part c I don't have much clue for. I tried just putting the hamiltonian into mathematica with that wave function, to see what it gives me, but it didn't give me anything that I can see looks like the RHS of the equation, any suggestions on how to go about part c would be appreciated.
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