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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

Analyze the Zeeman effect for the n=3states of hydrogen, in the weak, strong, and intermediate field regimes. Construct a table of energies (analogous to Table 6.2), plot them as functions of the external field (as in Figure 6.12), and check that the intermediate-field results reduce properly in the two limiting cases.

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).

Question: Consider a quantum system with just three linearly independent states. Suppose the Hamiltonian, in matrix form, is

H=V0(1-o˙0000o˙0o˙2)

WhereV0is a constant, ando˙is some small number(1).

(a) Write down the eigenvectors and eigenvalues of the unperturbed Hamiltonian(o˙=0).

(b) Solve for the exact eigen values of H. Expand each of them as a power series ino˙, up to second order.

(c) Use first- and second-order non degenerate perturbation theory to find the approximate eigen value for the state that grows out of the non-degenerate eigenvector ofH0. Compare the exact result, from (a).

(d) Use degenerate perturbation theory to find the first-order correction to the two initially degenerate eigen values. Compare the exact results.

Question: In Problem 4.43you calculated the expectation value ofrsin the stateψ321. Check your answer for the special cases s = 0(trivial), s = -1(Equation 6.55), s = -2(Equation 6.56), and s = -3(Equation 6.64). Comment on the case s = -7.

Consider the isotropic three-dimensional harmonic oscillator (Problem 4.38). Discuss the effect (in first order) of the perturbation H'=λx2yz

(for some constant λ) on

(a) the ground state

(b) the (triply degenerate) first excited state. Hint: Use the answers to Problems 2.12and 3.33

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