Electron Spin — Question 5

Section 40-2 · Physics pages 6600–6601

Question 5 A transverse measurement saturates the spin uncertainty bound An electron is in | + z⟩. Use S2 x = S2 y = S2 z = ℏ2I/4, ⟨Sx⟩= ⟨Sy⟩= 0, and [Sx, Sy] = iℏSz. z x ˆn θ Schematic; labels, not drawing lengths, specify the data. (a) Calculate both transverse standard deviations. (b) Compare their product with 1 2|⟨[Sx, Sy]⟩|.
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Question 5 - Solution A transverse measurement saturates the spin uncertainty bound z x ˆn θ (a) Method and calculation (∆Sx)2 = ⟨S2 x⟩−⟨Sx⟩2 = ℏ2/4. ∆Sx = ∆Sy = ℏ/2 . (b) Interpretation and further calculation ∆Sx∆Sy = ℏ2/4. 1 2|iℏ⟨Sz⟩| = ℏ2/4 ⇒bound saturated . Physical check A precisely known z projection does not make transverse measurements precise. This uncertainty describes repeated measurements on identically prepared electrons.

Question 5

A transverse measurement saturates the spin uncertainty bound

An electron is in |+z⟩|+z\rangle. Use Sx2=Sy2=Sz2=ℏ2I/4S_x^2=S_y^2=S_z^2=\hbar^2 I/4, ⟨Sx⟩=⟨Sy⟩=0\langle S_x\rangle=\langle S_y\rangle=0, and [Sx,Sy]=iℏSz[S_x,S_y]=i\hbar S_z.

Diagram shown in the original SVG worksheet.

  1. Calculate both transverse standard deviations.

  2. Compare their product with 12|⟨[Sx,Sy]⟩|\frac12|\langle[S_x,S_y]\rangle|.

Question 5 - Solution

A transverse measurement saturates the spin uncertainty bound

Diagram shown in the original SVG worksheet.

(a) Method and calculation

(ΔSx)2=⟨Sx2⟩−⟨Sx⟩2=ℏ2/4.(\Delta S_x)^2=\langle S_x^2\rangle-\langle S_x\rangle^2=\hbar^2/4.ΔSx=ΔSy=ℏ/2.\boxed{\Delta S_x=\Delta S_y=\hbar/2}.

(b) Interpretation and further calculation

ΔSxΔSy=ℏ2/4.\Delta S_x\Delta S_y=\hbar^2/4.12|iℏ⟨Sz⟩|=ℏ2/4⇒bound saturated.\tfrac12|i\hbar\langle S_z\rangle|=\hbar^2/4\Rightarrow\boxed{\text{bound saturated}}.

Physical check

A precisely known z projection does not make transverse measurements precise. This uncertainty describes repeated measurements on identically prepared electrons.