Spin Prob 1: Difference between revisions

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(c) How could the difference between P and Q be detected experimentally?
(c) How could the difference between P and Q be detected experimentally?


Solution:
Solution:


(a) The spin state function <math>\psi_{p}</math> of P is the eigenfunction of <math>\S_{x}</math> with eigenvalue <math>+\frac{\hbar}{2}</math>. So <math>\psi_{p}=\frac{\alpha+\beta}{\root{2}}</math>
(a) The spin state function <math>\psi_{p}</math> of P is the eigenfunction of <math>S_{x}</math> with eigenvalue <math>+\frac{\hbar}{2}</math>. So <math>\psi_{p}=\frac{\alpha+\beta}{\sqrt{2}}</math>
 
(b) No. In each case the two beams emerging from the Stern-Gerlach apparatus would contain equal numbers of atoms.
 
 
(c) The difference between P and Q could be determined by passing each beam through a Stern-Gerlach magnet with its magnetic field along the x axis. For beam P all the atoms would emerge in the same channel, corresponding to x-component of spin angular momentum equal to <math>+\frac{\hbar}{2}</math>. For beam Q two beams would emerge with equal numbers of atoms. For this beam the same result would occur whatever the direction of the magnetic field of the Stern-Gerlach magnet.

Latest revision as of 00:47, 29 April 2010

Problem 1:(Added by Hang Chen's group)

P is a beam of atoms with spin quantum number 1/2 and zero orbital angular momentum, all with angular momentum along the x axis. Q is a beam of similar but unpolarised atoms.

(a) What's the spin state function of P in terms of and , the eigenfunctions of ?

(b) If the two beams are passed separately through a Stern-Gerlach apparatus with its magnetic field along the z axis, is there any difference between the emerging beams in the two cases?

(c) How could the difference between P and Q be detected experimentally?


Solution:

(a) The spin state function of P is the eigenfunction of with eigenvalue . So

(b) No. In each case the two beams emerging from the Stern-Gerlach apparatus would contain equal numbers of atoms.


(c) The difference between P and Q could be determined by passing each beam through a Stern-Gerlach magnet with its magnetic field along the x axis. For beam P all the atoms would emerge in the same channel, corresponding to x-component of spin angular momentum equal to . For beam Q two beams would emerge with equal numbers of atoms. For this beam the same result would occur whatever the direction of the magnetic field of the Stern-Gerlach magnet.