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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 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

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>

Problem 6.6 Let the two "good" unperturbed states be

ψ±0=α±ψa0+β±ψb0

whereα±andβ±are determined (up to normalization) by Equation 6.22(orEquation6.24). Show explicitly that

(a)are orthogonal;role="math" localid="1655966589608" (ψ+0ψ-0=0);

(b) ψ+0|H'|ψ-0=0;

(c)ψ±0|H'|ψ±0=E±1,withE±1given by Equation 6.27.

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

(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.

Consider a particle of mass m that is free to move in a one-dimensional region of length L that closes on itself (for instance, a bead that slides frictionlessly on a circular wire of circumference L, as inProblem 2.46).

(a) Show that the stationary states can be written in the formψn(x)=1Le2πinx/L,(-L/2<x<L/2),

wheren=0,±1,±2,....and the allowed energies areEn=2mnπL2.Notice that with the exception of the ground state (n = 0 ) – are all doubly degenerate.

(b) Now suppose we introduce the perturbation,H'=-V0e-x2/a2where aLa. (This puts a little “dimple” in the potential at x = 0, as though we bent the wire slightly to make a “trap”.) Find the first-order correction to En, using Equation 6.27. Hint: To evaluate the integrals, exploit the fact that aLato extend the limits from ±L/2to±after all, H′ is essentially zero outside -a<x<a.

E±1=12Waa+Wbb±Waa-Wbb2+4Wab2(6.27).

(c) What are the “good” linear combinations ofψnandψ-n, for this problem? Show that with these states you get the first-order correction using Equation 6.9.

En'=ψn0H'ψn0(6.9).

(d) Find a hermitian operator A that fits the requirements of the theorem, and show that the simultaneous Eigenstates ofH0and A are precisely the ones you used in (c).

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