Determine the commutator of S2withSZ(1)(whereSS(1)+S(2)) Generalize your result to show that

[S2,S1]=2Ih(S1×S2)

Comment: Because Sz(1)does not commute with S2, we cannot hope to find states that are simultaneous eigenvectors of both. In order to form eigenstates ofS2weneed linear combinations of eigenstates ofSz(1). This is precisely what the Clebsch-Gordan coefficients (in Equation 4.185) do for us, On the other hand, it follows by obvious inference from Equation 4.187that the sumrole="math" localid="1655980965321" S(1)+S(2)does commute withdata-custom-editor="chemistry" S2, which is a special case of something we already knew (see Equation 4.103).

Short Answer

Expert verified

S2,Sz1=2ihSx1Sy2-Sy1Sx2Onemayapplythefollowinggeneralizationtotheresult:S2,S1=2ihS1×S2

Step by step solution

01

Define Eigenstate

A quantum state whose wave function is an eigenfunction of the linear operator that corresponds to an observable is called an eigenstate. When you measure that observable, the eigenvalue of that wave function is the quantity you see (the eigenvalue could be a vector quantity).

02

Determine the commutator of S2 with Sz(1)

Firstofall,letusexpandS2.S2=S1+S2.S1+S2=S1+S2+2S1.S2Then,S2,Sz1=S1+S2+251.S2,SZ1Here,basedonthecommutator'sdistributivity,write:S2,Sz1=S12Sz1+S2,z1+2S1.S2,Sz1Forthefirsttime,locatethecommutotorasfollows:S12,Sz1=Sx12+Sy12+Sz12Sz1=Sx12,Sz1+Sy12,Sz1+Sz12,Sz1

UsetheidentityAB,C=AB,C+A,CBtosimplifytheproblem.ofcourse,Sz1iscommutewithitselflikeanyotheroperator,soSz12,Sz1=0,thus,

S12,Sz1=Sx1Sx1,Sz1+Sx1,Sz1Sx1+Sy1Sy1,Sz1Sy1=Sx1-ihSy1+-ihSy1Sx1+Sy1ihSx1+ihSx1Sy1=0

Thus,S2,Sz1=2ihSx1Sy2-Sy1Sx2IfdothesameprocedureS2,Sx1andS2,Sy1,findthemtobe2ihSy1Sz2-Sz1Sy2and-2ihSx1Sz2-Sz1Sx2respectively,somakeageneralizationS2,S1=2ihS1×S2

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Most popular questions from this chapter

The electron in a hydrogen atom occupies the combined spin and position stateR211/3Y10χ++2/3Y11χ-

(a) If you measured the orbital angular momentum squared L2, what values might you get, and what is the probability of each?

(b) Same for the component of orbital angular momentum Lz.

(c) Same for the spin angular momentum squaredS2 .

(d) Same for the component of spin angular momentum Sz.

Let JL+Sbe the total angular momentum.

(e) If you measureddata-custom-editor="chemistry" J2 , what values might you get, and what is the probability of each?

(f) Same forJz .

(g) If you measured the position of the particle, what is the probability density for finding it atr , θ,ϕ ?

(h) If you measured both the component of the spin and the distance from the origin (note that these are compatible observables), what is the probability density for finding the particle with spin up and at radius ?

(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.)

Work out the radial wave functions R30,R31,andR32using the recursion formula. Don’t bother to normalize them.

Work out the normalization factor for the spherical harmonics, as follows. From Section 4.1.2we know that

Ylm=BlmeimϕPlmcosθ

the problem is to determine the factor (which I quoted, but did not derive, in Equation 4.32). Use Equations 4.120, 4.121, and 4.130to obtain a recursion

relation giving Blm+1 in terms of Blm. Solve it by induction on to get Blm up to an overall constant Cl, .Finally, use the result of Problem 4.22 to fix the constant. You may find the following formula for the derivative of an associated Legendre function useful:

1-x2dPlmdx=1-x2Plm+1-mxPlm [4.199]

Use separation of variables in Cartesian coordinates to solve infinite cubical well

V(x,y,z)=0if x,y,z are all between 0 to a;

V(x,y,z)=Otherwise

a) Find the stationary states and the corresponding energies

b) Call the distinct energies E1,E2,E3,..in the order of increasing energy. Findlocalid="1658127758806" E1,E2,E3,E4,E5,E6determine their degeneracies (that is, the number of different states that share the same energy). Comment: In one dimension degenerate bound states do not occur but in three dimensions they are very common.

c) What is the degeneracy of E14 and why is this case interesting?

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