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Transcript
QUANTUM PHYSICS I
PROBLEM SET 2
due October 3rd, before class
Semi-classical quantization for a polynomial potential
In class we discussed the quantization of circular orbits of an electron around a nucleus considering only the Coulomb
electrostatic force between the electron and the nucleus. Repeat the argument in the case of a modified interaction
between electron and nucleus: assume the potential between them is V (r) = rαn .
1. Write them the quantization of angular momentum rule (which is independent of the potential) and the “F =
ma”’ equation.
2. Determine the radii and energies of the allowed orbits
A first look at the Uncertainty Principle
2
Consider a particle described at some particular instant of time by the wave function ψ(x) = Ae−ax .
1. Determine A so ψ is normalized.
2. Compute hxi, hx2 i and σx2 = h(x − hxi)2 i.
3. Compute hpi, hp2 i and σp2 = h(p − hpi)2 i.
4. Show that by changing a one can make either σx2 or σp2 small, but not both at the same time. Compute σx σp .
Ehrenfest’s theorem
Prove that
∂
hpi =
∂t
∂V (x)
Ψ(x, t) −
Ψ(x, t).
∂x
−∞
Z
∞
∗
(1)
This result is one way to show that, under certain circumstances, macroscopic objects obey Newton’s law F = ma.
Describe in words the connection of the formula above with Newton’s law.