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) Plugs=0,s=2, and s=3into Kramers' relation (Equation 6.104) to obtain formulas for (r-1),(r),(r-2),and(r3). Note that you could continue indefinitely, to find any positive power.

(b) In the other direction, however, you hit a snag. Put in s=-1, and show that all you get is a relation between role="math" localid="1658216018740" (r-2)and(r-3).

(c) But if you can get (r-2)by some other means, you can apply the Kramers' relation to obtain the rest of the negative powers. Use Equation 6.56(which is derived in Problem 6.33) to determine (r-3) , and check your answer against Equation 6.64.

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)ΔE,and does not occur (of course) in ordinary hydrogen, muonic hydrogen, or muoniun.

Use Equation 6.59 to estimate the internal field in hydrogen, and characterize quantitatively a "strong" and "weak" Zeeman field.

Prove Kramers' relation:

sn2rs-(2s+1)ars-1+s4[(2l+1)2-s2]a2rs-2=0

Which relates the expectation values of rto three different powers (s,s-1,ands-2),for an electron in the state ψn/mof hydrogen. Hint: Rewrite the radial equation (Equation) in the form

u''=[l(l+1)r2-2ar+1n2a2]u

And use it to expressrole="math" localid="1658192415441" (ursu'')drin terms of (rs),(rs-1)and(rs-2). Then use integration by parts to reduce the second derivative. Show that (ursu'')dr=-(s/2)(rs-1)and(u'rsu')dr=-[2/s+1](u''rs+1u')dr. Take it from there.

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