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

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.

Van der Waals interaction. Consider two atoms a distanceapart. Because they are electrically neutral you might suppose there would be no force between them, but if they are polarizable there is in fact a weak attraction. To model this system, picture each atom as an electron (mass m , charge -e ) attached by a spring (spring constant k ) to the nucleus (charge +e ), as in Figure. We'll assume the nuclei are heavy, and essentially motionless. The Hamiltonian for the unperturbed system is

H0=12mp12+12kx12+12mp22+12kx22[6.96]

The Coulomb interaction between the atoms is

H'=14πϵ0(e2R-e2R-x1-e2R+x2+e2R-x1+x2 [6.97]

(a) Explain Equation6.97. Assuming that localid="1658203563220" |x1| and |x2|are both much less than, show that

localid="1658203513972" H'-e2x1x22πϵ0R3 [6.98]

(b) Show that the total Hamiltonian (Equationplus Equation) separates into two harmonic oscillator Hamiltonians:

H=[12mp+2+12(k-e22πϵ0R3x+2]+[+12mp-2+12(k+e22πϵ0R3x-2] [6.99]

under the change of variables

x±12(x1±x2) Which entails p±=12(p1±p2) [6.100]

(c) The ground state energy for this Hamiltonian is evidently

E=12(ω++ω-) Where ω±=k(e2/2πϵ0R3)m [6.101]

Without the Coulomb interaction it would have been E0=ħω0, where ω0=k/m. Assuming that, show that

ΔVE-E0-8m2ω03(e22πϵ0)21R6. [6.102]

Conclusion: There is an attractive potential between the atoms, proportional to the inverse sixth power of their separation. This is the van der Waals interaction between two neutral atoms.

(d) Now do the same calculation using second-order perturbation theory. Hint: The unperturbed states are of the form ψn1(x1)ψn2(x2), where ψn(x)is a one-particle oscillator wave function with mass mand spring constant k;ΔVis the second-order correction to the ground state energy, for the perturbation in Equation 6.98 (notice that the first-order correction is zero).

Show thatP2is Hermitian, butP4is not, for hydrogen states withl=0. Hint: For such statesψis independent ofθandϕ, so

localid="1656070791118" p2=-2r2ddr(r2ddr)

(Equation 4.13). Using integration by parts, show that

localid="1656069411605" <fp2g>=-4πh2(r2fdgdr-r2gdfdr)0+<p2fg>

Check that the boundary term vanishes forψn00, which goes like

ψn00~1π(na)3/2exp(-r/na)

near the origin. Now do the same forp4, and show that the boundary terms do not vanish. In fact:

<ψn00p4ψm00>=84a4(n-m)(nm)5/2+<p4ψn00ψm00>

Question: Evaluate the following commutators :

a)[L·S,L]

b)[L·S,S]

c)role="math" localid="1658226147021" [L·S,J]

d)[L·S,L2]

e)[L·S,S2]

f)[L·S,J2]

Hint: L and S satisfy the fundamental commutation relations for angular momentum (Equations 4.99 and 4.134 ), but they commute with each other.

[LX,LY]=ihLz;[Ly,Lz]=ihLx;[Lz,Lx]=ihLy.......4.99[SX,SY]=ihSz;[Sy,Sz]=ihSx;[Sz,Sx]=ihSy........4.134

Question: The most prominent feature of the hydrogen spectrum in the visible region is the red Balmer line, coming from the transition n = 3to n = 2. First of all, determine the wavelength and frequency of this line according to the Bohr Theory. Fine structure splits this line into several closely spaced lines; the question is: How many, and what is their spacing? Hint: First determine how many sublevels the n = 2level splits into, and find Efs1for each of these, in eV. Then do the same for n = 3. Draw an energy level diagram showing all possible transitions from n = 3to n = 2. The energy released (in the form of a photon) is role="math" localid="1658311193797" (E3-E2)+E, the first part being common to all of them, and the E(due to fine structure) varying from one transition to the next. Find E(in eV) for each transition. Finally, convert to photon frequency, and determine the spacing between adjacent spectral lines (in Hz- -not the frequency interval between each line and the unperturbed line (which is, of course, unobservable), but the frequency interval between each line and the next one. Your final answer should take the form: "The red Balmer line splits into (???)lines. In order of increasing frequency, they come from the transitionsto (1) j =(???),toj =(???) ,(2) j =(???) to j =(???)……. The frequency spacing between line (1)and line (2)is (???) Hz, the spacing between line (2)and (3) line (???) Hzis……..”

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