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

Short Answer

Expert verified

The value ofY22θ,ϕis14152πheiϕsinθ2.

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 Y21θ,ϕ.

From problem 4.3, the value of Y21

Y21=-158ττsinθcosθeioL+=heiϕθ+icotθϕL+Y21=Y22

Now, determine the spherical harmonic Y22θ,ϕas follows,

localid="1658464225727" Y21=-158πheiϕeiϕ)(sinθcosθ)θ+icotθsinθcosθeiϕϕ=-158πheiϕeiϕ(cos2θ-sin2θ)+icotθsinθcosθ(ieiϕ)=-158πheiϕcos2θ-cos2θeiϕ=152πhe2iϕsin2θ=12152πh(e2iϕsinθ)2

Thus, the value ofY22θ,ϕislocalid="1658464244244" 12152πheiϕsin2θ2.

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Most popular questions from this chapter

An electron is at rest in an oscillating magnetic field

B=B0cos(ωt)k^

whereB0 andω 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:χ(0)=χ+(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 Schrödinger equation (Equation 4.162) directly.

(c) Find the probability of getting-h/2 , if you measure Sx. Answer:

sin2(γB02ωsin(ωt))

(d) What is the minimum field(B0) required to force a complete flip inSx ?

(a)Derive Equation 4.131 from Equation 4.130. Hint: Use a test function; otherwise you're likely to drop some terms.

(b)Derive Equation 4.132 from Equations 4.129 and 4.131 .Hint : Use Equation 4.112.

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]

(a) Find the eigenvalues and eigenspinors of Sy .

(b) If you measured Syon a particle in the general state X(Equation 4.139), what values might you get, and what is the probability of each? Check that the probabilities add up to 1 . Note: a and b need not be real!

(c) If you measuredSy2 , what values might you get, and with what probabilities?

(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.

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