Question: The exact fine-structure formula for hydrogen (obtained from the Dirac equation without recourse to perturbation theory) is 16

Enj=mc2{1+an-j+12+j+122-a22-12-1}

Expand to order α4(noting that α1), and show that you recoverEquation .

Short Answer

Expert verified

The recovered equation 6.67 is.Enj=-13.6n21+a2n2nj+12-34

Step by step solution

01

Formula Used

The exact fine structure formula for Hydrogen is:

Enj=mc2{1+an-j+12+j+122-a2212-1}

02

Use of Taylor Expansion

To expand w.r.t. , use Taylor expansion, first arrange the function, the term:

j+122-a2=j+121-aj+122

Now, expand this term by Taylor expansion:

Choose,x0=0,x=aj+12&f(x)1-aj+122

f(x)=f(x0)+(x-x0)f'(x)x-x0+x-x02!f(x)x-x0+...ddx1-x2=-2x21-x2f(x)x-x0=zero

And,

d2dx21-x2=-1-x2-12+x2-1-x2-32.(-2x)=-11-x2-x21-x232f"(x)|x-x0=-1-zero=-1

Use Taylor expansion

1-x2=1+x1!f'(x)|x-x0+x22!f"(x)|x-x0+...1+zero+x22!(-1)+...1-x2=1-x22

Then,

j+122-a2=j+121-aj+122j+121-12aj+122j+12-12a2j+12

03

Write the full term

Now, write the full terms as:

an-j+12j+122-a22an-j+12+j+12-a22j+122an-a22j+122

04

Expand the term and rearrange

Expand the term:

an-a22j+12

First, re-arrange that term:

αn11-n-a22nj+12=αn1-a22nj+12-1

Take,

x=a22nj+12f(x)=11-x',x0=0f'(x)=11-x2f'(x)|x-x0=1

And,

f'(x)=-21-x-11-x4=2-2x1-x4f"(x)|x-x0=2

Solve further

11-x=f(x0)+x1!f'(x)|x-x0+x22!f"(x)|x-x01+x+x211-x1+x

Then,

αn1-a22nj+12-1αn1+a22nj+12

05

The fine structure form

Now, write:

an-a22nj+122αn1+a22nj+122

Now, the exact fine structure can take the form:

1+αn1+a22nj+12212-1

06

Preserve the order

Preserve the order α4, so

width="359">αn1+a22nj+122=α2n21+a22nj+12+0(a4)α2n21+a2nj+12

Now, expand the term,

1+α2n21+a2nj+12-12

Take:

x=α2n21+a2nj+12,x0=0f(x)=11+x=1+x-12f'(x)=-12(1+x)-32 f'(x)|x-x0=-12f"(x)=34(1+x)-52f'(x)|x-x0=34f(x)=1+x1!-12+x22!34+...f(x)1-12x+38x21+α2n21+a2nj+12-12

Solve further,

1-12α2n21+a2nj+12+38α4n41+a2nj+121-12α2n21+a2nj+12+38α4n4+0(a6)

07

Find equation 6.67

Then,

Emjmc21-12α2n21+a2nj+12+38α4n4-1-mc2a22n21+a2nj+12+38α2n2-mc2a22n21+a2n2nj+12-34

α=1137.036mc2=0.511MeVEnj=-13.6n21+a2n2nj+12-34

As the same as equation (6.67).

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Most popular questions from this chapter

Two identical spin-zero bosons are placed in an infinite square well (Equation 2.19). They interact weakly with one another, via the potential

V(x1,x2)=-aV0δ(x1-x2). (2.19).

(where V0is a constant with the dimensions of energy, and a is the width of the well).

(a)First, ignoring the interaction between the particles, find the ground state and the first excited state—both the wave functions and the associated energies.

(b) Use first-order perturbation theory to estimate the effect of the particle– particle interaction on the energies of the ground state and the first excited state.

(a) Find the second-order correction to the energies(En2)for the potential in Problem 6.1. Comment: You can sum the series explicitly, obtaining -for odd n.

(b) Calculate the second-order correction to the ground state energy(E02)for the potential in Problem 6.2. Check that your result is consistent with the exact solution.

Question: In the text I asserted that the first-order corrections to an n-fold degenerate energy are the eigen values of the Wmatrix, and I justified this claim as the "natural" generalization of the case n = 2.

Prove it, by reproducing the steps in Section 6.2.1, starting with

ψ0=j=1nαjψj0

(generalizing Equation 6.17), and ending by showing that the analog to Equation6.22 can be interpreted as the eigen value equation for the matrix W.

Question: Use the virial theorem (Problem 4.40) to prove Equation 6.55.

Question: Consider the Stark effect (Problem 6.36) for the states of hydrogen. There are initially nine degenerate states, ψ3/m (neglecting spin, as before), and we turn on an electric field in the direction.

(a) Construct the matrix representing the perturbing Hamiltonian. Partial answer: <300|z|310>=-36a,<310|z|320>=-33a,<31±1|z|32±1>=-(9/2)a,,

(b) Find the eigenvalues, and their degeneracies.

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