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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 α≪1), 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-x232⇒f"(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+122≈j+121-12aj+122≈j+12-12a2j+12

03

Write the full term

Now, write the full terms as:

an-j+12j+122-a22≈an-j+12+j+12-a22j+122≈an-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+12⇒f(x)=11-x',x0=0f'(x)=11-x2⇒f'(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-x0≈1+x+x2⇒11-x≈1+x

Then,

αn1-a22nj+12-1≈αn1+a22nj+12

05

The fine structure form

Now, write:

an-a22nj+122≈αn1+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)-52⇒f'(x)|x-x0=34f(x)=1+x1!-12+x22!34+...f(x)≈1-12x+38x2⇒1+α2n21+a2nj+12-12

Solve further,

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

07

Find equation 6.67

Then,

Emj≈mc21-12α2n21+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

By appropriate modification of the hydrogen formula, determine the hyperfine splitting in the ground state of

(a) muonic hydrogen (in which a muon-same charge and g-factor as the electron, but 207times the mass-substitutes for the electron),

(b) positronium (in which a positron-same mass and g-factor as the electron, but opposite charge-substitutes for the proton), and

(c) muonium (in which an anti-muon-same mass and g-factor as a muon, but opposite charge-substitutes for the proton). Hint: Don't forget to use the reduced mass (Problem 5.1) in calculating the "Bohr radius" of these exotic "atoms." Incidentally, the answer you get for positronium (4.82×10-4eV)is quite far from the experimental value; (8.41×10-4eV)the large discrepancy is due to pair annihilation (e++e-→γ+γ), which contributes an extra localid="1656057412048" (3/4)Δ·¡,and does not occur (of course) in ordinary hydrogen, muonic hydrogen, or muoniun.

Consider the (eight) n=2states,|2lmlms⟩.Find the energy of each state, under strong-field Zeeman splitting. Express each answer as the sum of three terms: the Bohr energy, the fine-structure (proportional toa2), and the Zeeman contribution (proportional toμBBext.). If you ignore fine structure altogether, how many distinct levels are there, and what are their degeneracies?

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

Question: Derive the fine structure formula (Equation 6.66) from the relativistic correction (Equation 6.57) and the spin-orbit coupling (Equation 6.65). Hint: Note tha j=l±12t; treat the plus sign and the minus sign separately, and you'll find that you get the same final answer either way.

If I=0, then j=s,mj=ms, and the "good" states are the same (nms)for weak and strong fields. DetermineEz1(from Equation) and the fine structure energies (Equation 6.67), and write down the general result for the I=O Zeeman Effect - regardless of the strength of the field. Show that the strong field formula (Equation 6.82) reproduces this result, provided that we interpret the indeterminate term in square brackets as.

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