(a) Use Eqn. (2.41) or (2.40) to find the eigenvectors and eigenvalues of a spin measurement aligned at a 45 degree from both the x- and z- axes (in the x-z plane; no y component). (b) Suppose you carry out this measurement on a spin-up state (|+)). What out- comes might you find, and which which probabilities for each? (c) Suppose the actual outcome is the least likely possibility, in one particular instance. After this measurement, you measure Sz. Now what might you find, and which which probabilities for each?

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(a) Use Eqn. (2.41) or (2.40) to find the eigenvectors and eigenvalues of a spin
measurement aligned at a 45 degree from both the x- and z- axes (in the x-Z
plane; no y component).
(b) Suppose you carry out this measurement on a spin-up state (|+)). What out-
comes might you find, and which which probabilities for each?
(c) Suppose the actual outcome is the least likely possibility, in one particular
instance. After this measurement, you measure S2. Now what might you find,
and which which probabilities for each?
Transcribed Image Text:(a) Use Eqn. (2.41) or (2.40) to find the eigenvectors and eigenvalues of a spin measurement aligned at a 45 degree from both the x- and z- axes (in the x-Z plane; no y component). (b) Suppose you carry out this measurement on a spin-up state (|+)). What out- comes might you find, and which which probabilities for each? (c) Suppose the actual outcome is the least likely possibility, in one particular instance. After this measurement, you measure S2. Now what might you find, and which which probabilities for each?
The spin component along this direction is obtained by projecting the spin vector S onto this new unit
vector
S, = S•în
(2.40)
S, sin 0 cos o + S, sin 0 sin + S¸ cos 0.
%3D
The matrix representations we found for S,, S,, and S, lead to the matrix representation of the spin
component operator S„ (Problem 2.6):
sin e e-iø
h ( cos0
S.
2 \sin0 e' -cos0
(2.41)
Transcribed Image Text:The spin component along this direction is obtained by projecting the spin vector S onto this new unit vector S, = S•în (2.40) S, sin 0 cos o + S, sin 0 sin + S¸ cos 0. %3D The matrix representations we found for S,, S,, and S, lead to the matrix representation of the spin component operator S„ (Problem 2.6): sin e e-iø h ( cos0 S. 2 \sin0 e' -cos0 (2.41)
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