Work out the matrix elements of HZ'andHfs'construct the W matrix given in the text, for n = 2.

Short Answer

Expert verified

Hz'11=β;Hz'22=-β;Hz'33=2β;Hz'44=-2β.

,Hz'55=(2/3)β,Hz'66=(1/3)β,Hz'77=-(2/3)β,Hz'88=-(1/3)β,Hz'56=Hz'65=-(2/3)β,Hz'78=Hz'87=-(2/3)β

Step by step solution

01

Using Fine-Structure Formula.

We get the complete Fine-Structure Formula is,

Efs1=En22mc23-4nj+1/2

02

Working out the matrix elements of HZ' and Hfs' .

Using Equation 6:66,

Efs1=E222mc23-8j+1/2=E1232mc23-8j+1/2;E1mc2=-α22,

So.

Efs1=-E132α223-8j+1/2=13.6eV64α23-8j+1/2=γ3-8j+1/2.

Efs1=En22mc23-4nj+1/2

For

j=1/2ψ1,ψ2,ψ6,ψ8Hfs1=γ(3-8)Hfs1=-5γ.

Forj=3/2ψ3,ψ4,ψ5,ψ7

Hfs1=γ3-82Hfs1=-γ

This confirms all the γ terms in -W (p. 281).

Meanwhile, Hz'=(e/2m)BextLz+2Sz,ψ1,ψ2,ψ3,ψ4are Eigen states of LzandSz for these there are only diagonal elements:

HZ'=e2m(L+2S)·Bext

Hz'=e2mBextml+2msHz'=ml+2msβ;Hz'11=β;Hz'22=-β;Hz'33=2β;Hz'44=-2β.

This confirms the upper left corner of -W.

Finally:

Lz+2Szψ5=+23|101212Lz+2Szψ6=-13|101212Lz+2Szψ7=-23|1012-12Lz+2Szψ8=-13|1012-12so,Hz'55=(2/3)β,Hz'66=(1/3)β,Hz'77=-(2/3)β,Hz'88=-(1/3)β,Hz'56=Hz'65=-(2/3)β,Hz'78=Hz'87=-(2/3)β

which confirms the remaining elements.

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Most popular questions from this chapter

The Feynman-Hellmann theorem (Problem 6.32) can be used to determine the expectation values of1/rand1/r2for hydrogen.23The effective Hamiltonian for the radial wave functions is (Equation4.53)

22md2dr2+22ml(l+1)r2-e24π01r

And the eigenvalues (expressed in terms ofl)24are (Equation 4.70)

En=-me432π202h2jmax+l+12

(a) Use λ=ein the Feynman-Hellmann theorem to obtain 1/r. Check your result against Equation 6.55.

(b) Use λ=lto obtain 1/r2. Check your answer with Equation6.56.

Suppose the Hamiltonian H, for a particular quantum system, is a function of some parameter λlet En(λ)and ψn(λ)be the eigen values and

Eigen functions of. The Feynman-Hellmann theorem22states that

Enλ=(ψnHλψn)

(Assuming either that Enis nondegenerate, or-if degenerate-that the ψn's are the "good" linear combinations of the degenerate Eigen functions).

(a) Prove the Feynman-Hellmann theorem. Hint: Use Equation 6.9.

(b) Apply it to the one-dimensional harmonic oscillator,(i)using λ=ω(this yields a formula for the expectation value of V), (II)using λ=ħ(this yields (T)),and (iii)using λ=m(this yields a relation between (T)and (V)). Compare your answers to Problem 2.12, and the virial theorem predictions (Problem 3.31).

For the harmonic oscillator[Vx=1/2kx2], the allowed energies areEN=(n+1/2)ħω,(n=0.1.2,..),whererole="math" localid="1656044150836" ω=k/mis the classical frequency. Now suppose the spring constant increases slightly:k(1+ο')k(Perhaps we cool the spring, so it becomes less flexible.)

(a) Find the exact new energies (trivial, in this case). Expand your formula as a power series inο,, up to second order.

(b) Now calculate the first-order perturbation in the energy, using Equation 6.9. What ishere? Compare your result with part (a).

Hint: It is not necessary - in fact, it is not permitted - to calculate a single integral in doing this problem.

Suppose we perturb the infinite cubical well (Equation 6.30) by putting a delta function “bump” at the point(a/4,a/2,3a/4):H'=a3V0δ(x-a/4)δ(y-a/2)δ(z-3a/4).

Find the first-order corrections to the energy of the ground state and the (triply degenerate) first excited states.

Question: Sometimes it is possible to solve Equation 6.10 directly, without having to expand in terms of the unperturbed wave functions (Equation 6.11). Here are two particularly nice examples.

(a) Stark effect in the ground state of hydrogen.

(i) Find the first-order correction to the ground state of hydrogen in the presence of a uniform external electric fieldEext (the Stark effect-see Problem 6.36). Hint: Try a solution of the form

(A+Br+Cr2)e-r/acosθ

your problem is to find the constants , and C that solve Equation 6.10.

(ii) Use Equation to determine the second-order correction to the ground state energy (the first-order correction is zero, as you found in Problem 6.36(a)). Answer:-m(3a2eEext/2)2 .

(b) If the proton had an electric dipole moment p the potential energy of the electron in hydrogen would be perturbed in the amount

H'=-epcosθ4π̀o0r2

(i) Solve Equation 6.10 for the first-order correction to the ground state wave function.

(ii) Show that the total electric dipole moment of the atom is (surprisingly) zero, to this order.

(iii) Use Equation 6.14 to determine the second-order correction to the ground state energy. What is the first-order correction?

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