(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?

Short Answer

Expert verified
  1. The required eigenvalues are ±h2 and eigenspinors of Sy are 12i,12-i.
  2. The probability of each is 12a2+b2+iab*-ba*and 12a2+b2-iab*-ba*.
  3. The value of Sy2is h24and the probability is 1.

Step by step solution

01

Definition of probability

The theoretical probability of an event is the number of possible outcomes divided by the number of possible outcomes, with the probability being the chance of an outcome or event.

As a result, probability refers to the possibility or frequency with which something occurs.

02

(a) Determination of the eigenvalues and eigenspinors

Determine the eigenvalues in the following way.

-λ-ih2-ih2-λ=λ2-h24=0λ=±h2

Determine the eigenspinors in the following way.

Forλ=h2,

h20-ii0ab=h2abab=-ibia

So, b=iaand χn+~=aia.

It is known that a'χχn~=1.

a*-ia*aia=a2+a2=1a=12

So, χn+=121i~

Determine the eigenspinors in the following way.

Forλ=-h2,

h20-ii0ab=-h2ab-ab=-ibia

So, b=-ia, and |χn+~=a-ia.

It is known that a'χxn~=1.

a*-ia*a-ia=a2+a2=1a=12

So,|xn~-121-i.

Thus, the required eigenvalues are ±h2and eigenspinors of Sy are 12i,12-i.

03

(b) Determination of the probability

The likelihood of measuring ±h2 of Sy is obtained as follows,

P+y=χ+y|χ2=121-iab2=12a-ib2=12a2+b2+iab*-ba*

P-y=χ-y|χ2=121iab2=12a+ib2=12a2+b2-iab*-ba*

Add the probabilities.

P+y+P-y=a2+b2=a'χ|χn~=1

Thus, the probability of each is 12a2+b2+iab*-ba*and 12a2+b2-iab*-ba*.

04

(c) Determination of the value of Sy2 , with probability

The anticipated value ofSy2is obtained in the following way,

Sy2=h2410=h241χSy2χ=h24a'χ|χn~=h24

Thus, the value of Sy2 is h24and the probability is 1.

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Most popular questions from this chapter

The (time-independent) momentum space wave function in three dimensions is defined by the natural generalization of Equation 3.54:

Φ(p,t)=12πhe-ipx/hψ(x,t)dx(3.54).ϕ(p)1(2πh)3/2e-i(p.r)Ihψ(r)d3r.(4.223).

(a)Find the momentum space wave function for the ground state of hydrogen (Equation 4.80). Hint: Use spherical coordinates, setting the polar axis along the direction of p. Do the θ integral first. Answer:

ψ100(r,θ,ϕ)=1πa3e-r/a(4.80).ϕ(p)=1π(2ah)3/21[1+ap/h2]2.(4.224).

(b) Check that Φ(p)is normalized.

(c) Use Φ(p)to calculate <p2>, in the ground state of hydrogen.

(d) What is the expectation value of the kinetic energy in this state? Express your answer as a multiple of E1, and check that it is consistent with the virial theorem (Equation 4.218).

<T>=-En;<V>=2En(4.218).

Work out the spin matrices for arbitrary spin , generalizing spin (Equations 4.145 and 4.147), spin 1 (Problem 4.31), and spin (Problem 4.52). Answer:

Sz=(s0000s-10000s-200000-s)Sx=2(0bs0000bs0bs-10000bs-10bs-20000bs-200000000b-s+10000b-s+10)Sy=2(0-ibs0000ibs0-ibs-10000-ibs-10-ibs-20000-ibs-200000000-ibs+10000-ibs+10)

where,bj(s+j)(s+1-j)

(a) If you measured the component of spin angular momentum along the x direction, at time t, what is the probability that you would get +h/2?

(b) Same question, but for the ycomponent.

(c) Same, for the z component.

Two particles of mass mare attached to the ends of a massless rigid rod of length a. The system is free to rotate in three dimensions about the center (but the center point itself is fixed).

(a) Show that the allowed energies of this rigid rotor are

En=h2n(n+1)ma2, for n=0,1,2,...

Hint: First express the (classical) energy in terms of the total angular momentum.

(b) What are the normalized Eigen functions for this system? What is the degeneracy of thenthenergy level?

Construct the matrixSrrepresenting the component of spin angular momentum along an arbitrary directionr. Use spherical coordinates, for which

rsinθcosΦı+sinθsinΦø+cosθk [4.154]

Find the eigenvalues and (normalized) eigen spinors ofSr. Answer:

x+(r)=(cosθ/2esinθ/2); x+(r)=(esin(θ/2)-cos(θ/2)) [4.155]

Note: You're always free to multiply by an arbitrary phase factor-say,eiϕ-so your answer may not look exactly the same as mine.

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