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Construct the spin matrices(Sx,Sy鈥塧苍诲Sz) , 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(m1)|s(m1)

02

 Step 2: Construct spin matrice  Sz

For spin 1 particles, the eigen spinors are :

|+=(100)|0=(010)|=(001)

S|sm=s(s+1)m(m1)|s(m1) ...(4.136)

Sz+=+Sz0=0Sz=

From Equation 4.136

Sz=(100000001)

03

 Step 3: Construct spin matrice  Sx

S++=0S+=20S+0=2+.

S+=20S0=2S=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) Construct the wave function for hydrogen in the state n=4,I=3,m=3. Express your answer as a function of the spherical coordinates r,and.

(b) Find the expectation value of role="math" localid="1658391074946" rin this state. (As always, look up any nontrivial integrals.)

(c) If you could somehow measure the observable Lx2+Ly2on an atom in this state, what value (or values) could you get, and what is the probability of each?

(a) NormalizeR20 (Equation 4.82), and construct the function200.

(b) NormalizeR21(Equation 4.83), and construct the function.

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

(p,t)=12he-ipx/h(x,t)dx(3.54).(p)1(2h)3/2e-i(p.r)Ih(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 胃 integral first. Answer:

100(r,,)=1蟺补3e-r/a(4.80).(p)=1(2ah)3/21[1+ap/h2]2.(4.224).

(b) Check that (p)is normalized.

(c) Use (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).

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 ?

Consider the three-dimensional harmonic oscillator, for which the potential is

V(r)=12m蝇2r2

(a) Show that separation of variables in cartesian coordinates turns this into three one-dimensional oscillators, and exploit your knowledge of the latter to determine the allowed energies. Answer:

En=(n+3/2)h

(b) Determine the degeneracyofd(n)ofEn.

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