Electrons and Matter Waves — Question 9

Section 38-5 · Physics pages 6348–6349

Question 9 Matter wavelength changes under a Galilean change of reference frame A nonrelativistic particle has laboratory momentum p = mv > 0 and wavelength λ = h/(mv). An observer moves along +x at speed u; momentum in that frame is p′ = m(v −u). Define wavelength using the magnitude of momentum. x v u Schematic; labels, not drawing lengths, specify the data. (a) Find the wavelength and propagation direction for u = v/2 and u = 2v. (b) Interpret the plane-wave state in the frame u = v.
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Question 9 - Solution Matter wavelength changes under a Galilean change of reference frame x v u (a) Method and calculation u = v/2 : p′ = mv/2, λ′ = 2λ, direction + x . u = 2v : p′ = −mv, λ′ = λ, direction −x . (b) Interpretation and further calculation u = v : p′ = 0, k′ = 0 . ψ′(x′) ∝eik′x′ = 1, λ′ →∞. Physical check This is a delocalized momentum eigenstate, not an assertion that a material object has infinite size. A physical localized packet has a range of momenta.

Question 9

Matter wavelength changes under a Galilean change of reference frame

A nonrelativistic particle has laboratory momentum p=mv>0p=mv>0 and wavelength λ=h/(mv)\lambda=h/(mv). An observer moves along +x at speed uu; momentum in that frame is p′=m(v−u)p\prime=m(v-u). Define wavelength using the magnitude of momentum.

Diagram shown in the original SVG worksheet.

  1. Find the wavelength and propagation direction for u=v/2u=v/2 and u=2vu=2v.

  2. Interpret the plane-wave state in the frame u=vu=v.

Question 9 - Solution

Matter wavelength changes under a Galilean change of reference frame

Diagram shown in the original SVG worksheet.

(a) Method and calculation

u=v/2:p′=mv/2,λ′=2λ,direction +x.u=v/2:\quad p\prime=mv/2,\quad\boxed{\lambda\prime=2\lambda,\quad\text{direction }+x}.u=2v:p′=−mv,λ′=λ,direction −x.u=2v:\quad p\prime=-mv,\quad\boxed{\lambda\prime=\lambda,\quad\text{direction }-x}.

(b) Interpretation and further calculation

u=v:p′=0,k′=0.u=v:\quad\boxed{p\prime=0,\quad k\prime=0}.ψ′(x′)∝eik′x′=1,λ′→∞.\psi\prime(x\prime)\propto e^{ik\prime x\prime}=1,\qquad\lambda\prime\to\infty.

Physical check

This is a delocalized momentum eigenstate, not an assertion that a material object has infinite size. A physical localized packet has a range of momenta.