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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

(a) From the definition (Equation 4.46), construct n1(x)andn2(x).

(b) Expand the sines and cosines to obtain approximate formulas forn1(x)androle="math" localid="1656329588644" n2(x), valid whenx1.. Confirm that they blow up at the origin.

(a) For a functionf(ϕ)that can be expanded in a Taylor series, show that f(ϕ+φ)=eiLzφ/f(ϕ) (where is an arbitrary angle). For this reason, Lz/ is called the generator of rotations about the Z-axis. Hint: Use Equation 4.129 , and refer Problem 3.39.More generally, L·n^/ is the generator of rotations about the direction n^, in the sense that exp(iL·n^φ/)effects a rotation through angleφ (in the right-hand sense) about the axis n^ . In the case of spin, the generator of rotations is S·n^/. In particular, for spin 1/2 χ'=ei(σ·n^)φ/2χtells us how spinors rotate.

(b) Construct the (2×2)matrix representing rotation by 180about the X-axis, and show that it converts "spin up" χ+into "spin down"χ- , as you would expect.

(c) Construct the matrix representing rotation by 90about the Y-axis, and check what it does to

χ+

(d) Construct the matrix representing rotation by 360about the -Zaxis, If the answer is not quite what you expected, discuss its implications.

(e) Show thatei(σ·n^)φ/2=cos(φ/2)+i(n^·σ)sin(φ/2)

If the electron were a classical solid sphere, with radius

rc=e24πO0˙mc2

(the so-called classical electron radius, obtained by assuming the electron's mass is attributable to energy stored in its electric field, via the Einstein formula E=mc2), and its angular momentum is (1/2)h then how fast (in m/sm/s) would a point on the "equator" be moving? Does this model make sense? (Actually, the radius of the electron is known experimentally to be much less than5.156×1010m/src, but this only makes matters worse).

(a) Construct the spatial wave function (ψ)for hydrogen in the state n=3,I=2,m=1.Express your answer as a function of r,θ,ϕ,anda(the Bohr radius) only—no other variables (p,z,etc.) or functions (p,v,etc.), or constants (A,c0,etc.), or derivatives, allowed (π is okay, and e, and 2, etc.).

(b) Check that this wave function is properly normalized, by carrying out the appropriate integrals over, θ,andϕ.

(c) Find the expectation value of rsin this state. For what range of s (positive and negative) is the result finite?

Use equations 4.27 4.28 and 4.32 to construct Y00,Y21Check that they are normalized and orthogonal

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