Construct the spin matrices(Sx,Sy andSz) , for a particle of spin 1. Hint: How many eigenstates ofSz are there? Determine the action of Sz, S+, and Son each of these states. Follow the procedure used in the text for spin 1/2.

Short Answer

Expert verified

The matrices are Sx=2(010101010) Sy=i2(010101010)and Sz=(100000001)

Step by step solution

01

Important relations related to the solution

Important relations,

(1)Szis diagonal with its eigenvalues in the diagonal.

(2) Spin 1 particles havems=1,0,1.

(3) The eigenvalue ofSzfor spin 1 particles are:,0,.

(4) S±|sm=s(s+1)m(m±1)|s(m±1)

02

 Step 2: Construct spin matrice  Sz

For spin 1 particles, the eigen spinors are :

|χ+=(100)|χ0=(010)|χ=(001)

S±|sm=s(s+1)m(m±1)|s(m±1) ...(4.136)

Szχ+=χ+Szχ0=0Szχ=χ

From Equation 4.136

Sz=(100000001)

03

 Step 3: Construct spin matrice  Sx

S+χ+=0Sχ+=2χ0S+χ0=2χ+.

S+χ=2χ0Sχ0=2χSχ=0

S+=2(010001000)S=2(000100010)

Sx=12(S++S)=2(010101010)

04

Construct spin matrice  Sy

Sy=12i(S+S)=i2(010101010)

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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?

An electron is at rest in an oscillating magnetic field

B=B0cos(ωt)k^

whereB0 andω 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:χ(0)=χ+(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 Schrödinger equation (Equation 4.162) directly.

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

sin2(γB02ωsin(ωt))

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

Consider the observablesA=x2andB=Lz .

(a) Construct the uncertainty principle forσAσB

(b) EvaluateσB in the hydrogen stateψn/m .

(c) What can you conclude about<xy>in this state?

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.

[Attempt this problem only if you are familiar with vector calculus.] Define the (three-dimensional) probability current by generalization of Problem 1.14:

J=ih2m(ψψ*-ψ*ψ)

(a) Show that satisfies the continuity equation .J=-t|ψ|2which expresses local conservation of probability. It follows (from the divergence theorem) that sJ.da=-ddtv|ψ|2d3rwhere Vis a (fixed) volume and is its boundary surface. In words: The flow of probability out through the surface is equal to the decrease in probability of finding the particle in the volume.

(b) FindJfor hydrogen in the staten=2,l=1,m=1 . Answer:

h64ma5re-r/asinθϕ^

(c) If we interpretmJas the flow of mass, the angular momentum is

L=m(r×J)d3r

Use this to calculate Lzfor the stateψ211, and comment on the result.

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