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

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