A microscope is used to observe an electron

PHYSICS · Multi-part · A Level · Physics · Particles and radiation · Particles and radiation

Problem

A microscope is used to observe an electron. The objective of the microscope subtends a total angle 2θ2\theta at the scattering point, and the photon employed has wavelength λ\lambda. (i) Show that, due to diffraction at the aperture, the minimum uncertainty in the measured position of the electron perpendicular to the direction of observation is approximately Δx≈λ2sin⁡θ\Delta x \approx \dfrac{\lambda}{2\sin\theta}. (ii) Taking the transverse component of the photon’s momentum to be pγsin⁡θp_{\gamma}\sin\theta where pγ=hλp_{\gamma}=\dfrac{h}{\lambda}, prove that the uncertainty in the electron’s transverse momentum caused by the scattering is of the order Δp≈hsin⁡θλ\Delta p \approx \dfrac{h\sin\theta}{\lambda}. (iii) Hence derive that the product of the two uncertainties satisfies Δx Δp≳h4π\Delta x\,\Delta p \gtrsim \dfrac{h}{4\pi}, establishing the position–momentum uncertainty relation from this thought experiment.

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