Electrons and Matter Waves — Question 6

Section 38-5 · Physics pages 6342–6343

Question 6 The group velocity of a nonrelativistic matter wave follows the particle velocity A narrow packet has dispersion ω(k) = ℏk2/(2m) with k > 0. Define phase velocity vp = ω/k and group velocity vg = dω/dk. k ω Schematic; labels, not drawing lengths, specify the data. (a) Derive both velocities and relate them to momentum. (b) If a constant potential Vc is added, find the new velocities from ω = (ℏ2k2/2m + Vc)/ℏ.
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Question 6 - Solution The group velocity of a nonrelativistic matter wave follows the particle velocity k ω (a) Method and calculation vp = ℏk/(2m) = p/(2m) , vg = ℏk/m = p/m . vg = 2vp for the stated zero of potential energy. (b) Interpretation and further calculation v (c) p = ℏk 2m + Vc ℏk . v (c) g = dω dk = ℏk m . Physical check A constant energy offset changes the carrier phase rate but does not change packet transport or exert a force.

Question 6

The group velocity of a nonrelativistic matter wave follows the particle velocity

A narrow packet has dispersion ω(k)=ℏk2/(2m)\omega(k)=\hbar k^2/(2m) with k>0k>0. Define phase velocity vp=ω/kv_p=\omega/k and group velocity vg=dω/dkv_g=d\omega/dk.

Diagram shown in the original SVG worksheet.

  1. Derive both velocities and relate them to momentum.

  2. If a constant potential VcV_c is added, find the new velocities from ω=(ℏ2k2/2m+Vc)/ℏ\omega=(\hbar^2k^2/2m+V_c)/\hbar.

Question 6 - Solution

The group velocity of a nonrelativistic matter wave follows the particle velocity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

vp=ℏk/(2m)=p/(2m),vg=ℏk/m=p/m.\boxed{v_p=\hbar k/(2m)=p/(2m)},\qquad\boxed{v_g=\hbar k/m=p/m}.vg=2vpfor the stated zero of potential energy.\boxed{v_g=2v_p}\quad\text{for the stated zero of potential energy}.

(b) Interpretation and further calculation

vp(c)=ℏk2m+Vcℏk.\boxed{v_p^{\,(c)}=\frac{\hbar k}{2m}+\frac{V_c}{\hbar k}}.vg(c)=dωdk=ℏkm.\boxed{v_g^{\,(c)}=\frac{d\omega}{dk}=\frac{\hbar k}{m}}.

Physical check

A constant energy offset changes the carrier phase rate but does not change packet transport or exert a force.