QUANTUM PHYSICS I PROBLEM SET 5 - SOLUTION due November 10th before class

A. Muonic

A is a identical to an except its is about 200 times larger. A muonic hydrogen is a of a to a muon (instead of a proton and an electron as in the usual hydrogen). i) Use Bohr’s theory to calculate the energy levels of the muonic hydrogen. What is the energy of the (in eV ) ? We proceed as we (well, Bohr) did in the regular hydrogen . We use Newton’s law

e2 v2 2 = mµ (1) 4π0r

F ma | {z } and the Bohr quantization condition | {z }

L = mµvr = n~, (2) where n = 1, 2 · · · . Eliminating v in the first equation and plugging in the we can find r

2 4π0~ 2 rn = 2 n . (3) mµe The energy in each orbit can be found by 2 2 2 2 mµv e mµ e 1 mµ hydrogen En = − = − 2 2 = En ≈ 200 × (−13.6 eV ) ≈ −2.72keV, (4) 2 4π0r 2~ 4π0  n me where in the last step we restrict ourselves to the n = 1 case. Note that, in the calculation above, we assume that the nucleus does not move. Due to the difference in the of the proton and electron (mp ≈ 2000me) that was an excellent approximation for the . here, the difference between the proton and muon mass is not so large so this approximation is not so good. ii) Is the muon non-relativistic in the ground state of the muonic hydrogen ? The rest mass of the muon is about 200 × me ≈ 200 × 500 keV , which is much larger than the binding (or kinetic) energy of the muon in the muonic hydrogen. The muon is as non-relativistic here and the electron is in the hydrogen atom (there are, however relativistic corrections to the hydrogen spectrum and they are easily measured). iii) What is the wavelength of a emitted in a transition between the first and the ground state ? Which kind of photon is it ( radio, microwave, visible, ultraviolet, -ray, γ-ray, ...) ? The energy of the photon equals the difference in energy between the ground and first excited state 1 1 E = 2.72keV ( − ) ≈ 2.04keV. (5) γ 12 22 Using E = hν and λ = c/ν we find the wavelength to be hc λ = ≈ 0.6 nm, (6) E which is in the X-ray region. iv) Besides the mass, differ from electron by the fact that they “decay” into an electron and two massless, chargeless called “”. The lifetime for the decay is about 2 × 10−6s. Does the muon have the time to orbit the proton several times before decaying when it is in the ground state of muonic hydrogen ? The time it takes for the muon to go around one orbit is T = r/v. From 3 we find that v = n~/(mµr) so, for the ground state we have 2 2 3 −15 r m r 4π0~c 1 ~ 4.13/2π × 10 eV.s − T = = µ = ≈ (137)2 ≈ 6 × 10 15s >> muon lifetime. (7) ~ 2 ~2 2 6 eV 2 v  e  c mµ 1 × 10 c2 c 1/α2 | {z } 2

B. Operator wizardry

i) Show that the operator pˆ = −i~d/dx is an hermitian operator.

∞ ∞ ∞ ∗ d d ∗ d ∗ hf|pˆ|gi = dx f (x)(−i~ )g(x) = dx (i~ f (x))g(x) = dx (−i~ f(x)) g(x) = hpfˆ |gi. (8) Z−∞ dx Z−∞ dx Z−∞ dx

ii) Compute

− y ˆ e i ~ pf(x). (9)

Hint: expand the exponential and remember the Taylor series expression.

− y ˆ y 1 y 2 e i ~ pf(x) = (1 − i pˆ + (−i pˆ) + · · · )f(x) (10) ~ 2! ~ d 1 d = (1 − y + (−y )2 + · · · )f(x) (11) dx 2! dx 0 1 00 = f(x) − yf (x) + y2f (x) + · · · (12) 2! = f(x − y). (13)

ˆ iii) Show that Ψ(x, t) = e−iHt/~Ψ(x, 0) satisfies the Schr¨odinger equation. It is said that pˆ generates space transla- tions (from item ii) and Hˆ generates time translations (by item iii).

ˆ ∞ −iHt n d − ˆ ~ d ( ) i~ e iHt/ Ψ(x, 0) = i~ ~ Ψ(x, 0) (14) dt dt n! nX=0 ∞ ˆ ( −iHt )n−1 = nHˆ ~ Ψ(x, 0) (15) n! nX=1 ∞ ˆ 0 ( −iHt )n = Hˆ ~ Ψ(x, 0) (16) n0! nX0=0 − ˆ ~ = Hˆ e iHt/ Ψ(x, 0). (17)