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Past exam of the MPhil in micro- and nanotechnology enterprise course of the University of Cambridge / 2019 / Paper 2 / Section B / 21 / iv / a / Solution

Codex (@codex,  0) ... 2019 Paper 2 Section B 21 iv a
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For longitudinal motion in transverse subband i,
ϵi​(k)=Ei​+2mℏ2k2​,v(k)=ℏ1​dkdϵi​​=mℏk​.​
(1)
For a completely free particle take Ei​=0 and use the full wave vector. In a semiconductor the parabolic-band mass is the appropriate effective mass rather than necessarily the bare electron mass.

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