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An electron is in the spin state

=A3i4

(a) Determine the normalization constant .

(b) Find the expectation values of Sx,Sy , and Sz.

(c) Find the "uncertainties" ,Sx , SyandSz . (Note: These sigmas are standard deviations, not Pauli matrices!)

(d) Confirm that your results are consistent with all three uncertainty principles (Equation 4.100 and its cyclic permutations - only with in place ofL, of course).

Short Answer

Expert verified
  1. The normalization constant is A=15
  2. Theexpectation values of,, andis, and.
  3. Theexpectation values of,, andis, andrespectively
  4. The values of all three uncertainty principles , , and is , and .

Step by step solution

01

Significance of electron in spin state

The angular momentum of the electrons is used to describe the spin of the electrons. It only spins in two directions, that is up and down direction.

02

(a) Determine the normalization constant.

Determine the normalization constant by using =1

A2-3i43i4=1A2(9+16)=1A2=125A=15

Thus, the normalization constant is A=15

03

(b) Find the expectation values of Sx, Sy, and Sz

Determinethe expectation values of Sx.

Sx=Sx=50-3i401103i4=50-3i443i=5012i-12i

Determine theexpectation values ofSy.

Sy=Sy=50-3i40-ii03i4=50-3i4-4i3=50-12-12=-2450

Determine the expectation values ofSz

Sz=Sz=50-3i4100-13i4=50-3i43i-4=509-16=-750

Thus, the expectation values of Sx,Sy, and Szis 0, -2450 and-750

04

(c) Determination of the value of  σSx,σSy , and σSz

Determine the expectation values ofSx

dSx2=Sx2-Sx2Sx2=24-0Sx=2

Determine the expectation values of Sy.

Sy2=Sy2-Sy2Sy2=24-245022Sy2=4925002Sy=750

Determine the expectation values of Sz

Sz2=Sz2-Sz2Sz2=24-75022Sz2=57625002Sz=1225

Thus, the expectation values of Sx, Sy, and is 2, 750and 1225respectively

05

(d) Confirmation of the consistency of the results of all three uncertainty principles

Determine the value of SxSyto confirm the result.

SxSy=2750=2Sz=275

Determine the value of SySzto confirm the result.

SySz=7501225>2Sx=0

Determine the value of SzSxto confirm the result.

SzSx=12252=2Sy=21225

In general,SiSj2Sk and cyclic permutation.

Thus, the valuesof all three uncertainty principles SxSy, SySz, and SzSxis 275, 0 and 21225.

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Most popular questions from this chapter

(a) Find the eigenvalues and eigenspinors of Sy .

(b) If you measured Syon a particle in the general state X(Equation 4.139), what values might you get, and what is the probability of each? Check that the probabilities add up to 1 . Note: a and b need not be real!

(c) If you measuredSy2 , what values might you get, and with what probabilities?

What is the most probable value of r, in the ground state of hydrogen? (The answer is not zero!) Hint: First you must figure out the probability that the electron would be found between r and r + dr.

An electron is at rest in an oscillating magnetic field

B=B0cos(蝇迟)k^

whereB0 and are constants.

(a) Construct the Hamiltonian matrix for this system.

(b) The electron starts out (at t=0 ) in the spin-up state with respect to the x-axis (that is:(0)=+(x)). Determine X(t)at any subsequent time. Beware: This is a time-dependent Hamiltonian, so you cannot get in the usual way from stationary states. Fortunately, in this case you can solve the timedependent Schr枚dinger equation (Equation 4.162) directly.

(c) Find the probability of getting-h/2 , if you measure Sx. Answer:

sin2(纬叠02sin(蝇迟))

(d) What is the minimum field(B0) required to force a complete flip inSx ?

Use equations 4.27 4.28 and 4.32 to construct Y00,Y21Check that they are normalized and orthogonal

(a) Prove that for a particle in a potential V(r)the rate of change of the expectation value of the orbital angular momentum L is equal to the expectation value of the torque:

ddt<L>=<N>

Where,

N=r(VV)

(This is the rotational analog to Ehrenfest's theorem.)

(b) Show that d<L>/dt=0for any spherically symmetric potential. (This is one form of the quantum statement of conservation of angular momentum.)

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