Crossed Fields: The Hall Effect — Question 9

Section 28-4 · Physics pages 4548–4549

Question 9 A two-carrier material can have zero Hall voltage while conducting strongly For a weak-field electron-hole model, take the supplied relations σ = e(nµe + pµh) and RH = (pµ2 h −nµ2 e)/[e(pµh + nµe)2]. Here n,p are positive carrier densities and both mobilities are positive. electrons: n, µe holes: p, µh Schematic; labels, not drawing lengths, specify the data. (a) Find the condition for zero Hall coefficient with nonzero conductivity. (b) For µe = 2µh, find p/n at the Hall null and the corresponding conductivity. Explain why a Hall null does not establish absence of carriers.
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Question 9 - Solution A two-carrier material can have zero Hall voltage while conducting strongly electrons: n, µe holes: p, µh (a) Method and calculation RH = 0 ⇐⇒pµ2 h = nµ2 e ⇒p/n = (µe/µh)2. σ = e(nµe + pµh) > 0 for nonzero populations. (b) Interpretation and further calculation µe = 2µh ⇒p = 4n. σ = e(2nµh + 4nµh) = 6enµh. Physical check Hall contributions carry mobility-squared weights, so carrier-number majority alone does not determine the sign in this supplied model.

Question 9

A two-carrier material can have zero Hall voltage while conducting strongly

For a weak-field electron-hole model, take the supplied relations σ=e(nμe+pμh)\sigma=e(n\mu_e+p\mu_h) and RH=(pμh2−nμe2)/[e(pμh+nμe)2]R_H=(p\mu_h^2-n\mu_e^2)/[e(p\mu_h+n\mu_e)^2]. Here n,p are positive carrier densities and both mobilities are positive.

Diagram shown in the original SVG worksheet.

  1. Find the condition for zero Hall coefficient with nonzero conductivity.

  2. For μe=2μh\mu_e=2\mu_h, find p/n at the Hall null and the corresponding conductivity. Explain why a Hall null does not establish absence of carriers.

Question 9 - Solution

A two-carrier material can have zero Hall voltage while conducting strongly

Diagram shown in the original SVG worksheet.

(a) Method and calculation

RH=0⇔pμh2=nμe2⇒p/n=(μe/μh)2.R_H=0\Longleftrightarrow p\mu_h^2=n\mu_e^2\Rightarrow p/n=(\mu_e/\mu_h)^2.σ=e(nμe+pμh)>0for nonzero populations.\sigma=e(n\mu_e+p\mu_h)>0\quad\text{for nonzero populations}.

(b) Interpretation and further calculation

μe=2μh⇒p=4n.\mu_e=2\mu_h\Rightarrow p=4n.σ=e(2nμh+4nμh)=6enμh.\sigma=e(2n\mu_h+4n\mu_h)=6en\mu_h.

Physical check

Hall contributions carry mobility-squared weights, so carrier-number majority alone does not determine the sign in this supplied model.