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In Problem4.3 you showed that Y21(,)=-15/8sincosei. Apply the raising operator to find localid="1656065252558" Y22(,). Use Equation 4.121to get the normalization.

Short Answer

Expert verified

The value ofY22,is14152heisin2.

Step by step solution

01

Define Raising Operator

An operator that raises or lowers the eigenvalue of another operator (collectively called as ladder operators) is referred to as a raising or lowering operator.

02

Find the value of Y22(θ,ϕ)

In this step evaluate first the spherical harmonic is Y21,.

From problem 4.3, the value of Y21

Y21=-158sincoseioL+=hei+icotL+Y21=Y22

Now, determine the spherical harmonic Y22,as follows,

localid="1658464225727" Y21=-158heiei)(sincos)+icotsincosei=-158heiei(cos2-sin2)+icotsincos(iei)=-158heicos2-cos2ei=152he2isin2=12152h(e2isin)2

Thus, the value ofY22,islocalid="1658464244244" 12152heisin22.

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Most popular questions from this chapter

Work out the radial wave functions R30,R31,andR32using the recursion formula. Don鈥檛 bother to normalize them.

Work out the spin matrices for arbitrary spin , generalizing spin (Equations 4.145 and 4.147), spin 1 (Problem 4.31), and spin (Problem 4.52). Answer:

Sz=(s0000s-10000s-200000-s)Sx=2(0bs0000bs0bs-10000bs-10bs-20000bs-200000000b-s+10000b-s+10)Sy=2(0-ibs0000ibs0-ibs-10000-ibs-10-ibs-20000-ibs-200000000-ibs+10000-ibs+10)

where,bj(s+j)(s+1-j)

(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.)

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

[Refer to. Problem 4.59for background.] Suppose A=B02(X^-yI^) and=Kz2, where B0 and Kare constants.

(a) Find the fields E and B.

(b) Find the allowed energies, for a particle of mass m and charge q , in these fields, Answer: E(n1,n2)=(n1+12)1+(n2+12)2,(n1,n2=0,1,2,...)where1qB0/mand22qK/m. Comment: If K=0this is the quantum analog to cyclotron motion;1 is the classical cyclotron frequency, and it's a free particle in the z direction. The allowed energies,(n1+12)1, are called Landau Levels.

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