Chapter 2: Q18P (page 66)
Show that and are equivalent ways of writing the same function of , and determine the constants and in terms of and , and vice versa.
Short Answer
The constants and in terms of and , and vice versa are,
(i) and
(ii)
Chapter 2: Q18P (page 66)
Show that and are equivalent ways of writing the same function of , and determine the constants and in terms of and , and vice versa.
The constants and in terms of and , and vice versa are,
(i) and
(ii)
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Get started for free-consider the “step” potential:
a.Calculate the reflection coefficient, for the case E < V0, and comment on the answer.
b. Calculate the reflection coefficient, for the case E >V0.
c. For potential such as this, which does not go back to zero to the right of the barrier, the transmission coefficient is not simply (with A the incident amplitude and F the transmitted amplitude), because the transmitted wave travels at a different speed . Show that,for E >V0. What is T for E < V0?
d. For E > V0, calculate the transmission coefficient for the step potential, and check that T + R = 1.
Consider the potential 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
and find its energy. Normalize and sketch its graph.
(C)Show that the function
(Where as usual) solves the Schrödinger equation for any (positive) energy E. Sinceas This represents, then, a wave coming in from the left with no accompanying reflected wave (i.e., no term . What is the asymptotic form of 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.
In Problem 2.21 you analyzed the stationary gaussian free particle wave packet. Now solve the same problem for the traveling gaussian wave packet, starting with the initial wave function.
Find the transmission coefficient for the potential in problem 2.27
Solve the time-independent Schr ̈odinger equation for a centered infinite square well with a delta-function barrier in the middle:
Treat the even and odd wave functions separately. Don’t bother to normalize them. Find the allowed energies (graphically, if necessary). How do they compare with the corresponding energies in the absence of the delta function? Explain why the odd solutions are not affected by the delta function. Comment on the limiting cases α → 0 and α → ∞.
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