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?

Short Answer

Expert verified

Only five of the eight distinct energies remain when fine structure is ignored: There are three degenerate energies.

Step by step solution

01

Definition of Zeeman splitting.

When radiation (such as light) originates in a magnetic field, Zeeman splitting occurs, which is the splitting of a single spectral line into two or more lines of different frequencies.

02

Step2: Derivation.

For n=2, there are eight different states |2lmlms:

i)l=0ml=0ms=-12,ii)l=0ml=0ms=12,iii)l=1ml=-1ms=-12,iv)l=1ml=-1ms=12,v)l=1ml=0ms=-12,vi)l=1ml=0ms=12,vii)l=1ml=1ms=-12,viii)l=1ml=1ms=1/2i)l=0ml=0ms=-12,ii)l=0ml=0ms=12,iii)l=1ml=-1ms=-12,iv)l=1ml=-1ms=12,v)l=1ml=0ms=-12,vi)l=1ml=0ms=12,vii)l=1ml=1ms=-12,viii)l=1ml=1ms=12

Total energy is equal to:

E=-13.6eVn2+μBBext(ml+2ms)+13.6eVn3α234n-l(l+1)-mlmsll+12(l+1)

role="math" localid="1656064856692" i)E=-13.6eVn2-μBBext+13.6eVn3α234n-1.ii)E=-13.6eVn2+μBBext+13.6eVn3α234n-1.iii)E=-13.6eVn2-2μBBext+13.6eVn3α234n-32.iv)E=-13.6eVn2+13.6eVn3α234n-56.v)E=-13.6eVn2-μBBext+13.6eVn3α234n-23.vi)E=-13.6eVn2+μBBext+13.6eVn3α234n-23.vii)E=-13.6eVn2+2μBBext+13.6eVn3α234n-56.viii)E=-13.6eVn2+13.6eVn3α234n-12.

If fine structure is ignored,a=0.

Therefore, the following energies:

E=-13.6eVn2-μBBextDegree of degeneracy: 2

E=-13.6eVn2+μBBextDegree of degeneracy: 2

E=-13.6eVn2Degree of degeneracy: 2

E=-13.6eVn2-2μBBextDegree of degeneracy: 1

E=-13.6eVn2+2μBBextDegree of degeneracy: 1

Now only there are five distinct energies instead of eight.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

When an atom is placed in a uniform external electric field ,the energy levels are shifted-a phenomenon known as the Stark effect (it is the electrical analog to the Zeeman effect). In this problem we analyse the Stark effect for the n=1 and n=2 states of hydrogen. Let the field point in the z direction, so the potential energy of the electron is

H's=eEextz=eEextrcosθ

Treat this as a perturbation on the Bohr Hamiltonian (Equation 6.42). (Spin is irrelevant to this problem, so ignore it, and neglect the fine structure.)

(a) Show that the ground state energy is not affected by this perturbation, in first order.

(b) The first excited state is 4-fold degenerate: Y200,Y211,Y210,Y200,Y21-1Using degenerate perturbation theory, determine the first order corrections to the energy. Into how many levels does E2 split?

(c) What are the "good" wave functions for part (b)? Find the expectation value of the electric dipole moment (pe=-er) in each of these "good" states.Notice that the results are independent of the applied field-evidently hydrogen in its first excited state can carry a permanent electric dipole moment.

Sometimes it is possible to solve Equation 6.10 directly, without having to expand ψ1nin terms of the unperturbed wave functions (Equation 6.11). Here are two particularly nice examples.

(a) Stark effect in the ground state of hydrogen.

(i) Find the first-order correction to the ground state of hydrogen in the presence of a uniform external electric field (the Stark effect-see Problem 6.36). Hint: Try a solution of the form

(A+Br+Cr2)e-r/acosθ

your problem is to find the constants , and C that solve Equation 6.10.

(ii) Use Equation to determine the second-order correction to the ground state energy (the first-order correction is zero, as you found in Problem 6.36(a)).

Answer:-m(3a2eEext/2h)2

(b) If the proton had an electric dipole moment p the potential energy of the electron in hydrogen would be perturbed in the amount

H'=-epcosθ4π00r2~

(i) Solve Equation 6.10 for the first-order correction to the ground state wave function.

(ii) Show that the total electric dipole moment of the atom is (surprisingly) zero, to this order.

(iii) Use Equation 6.14 to determine the second-order correction to the ground state energy. What is the first-order correction?

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.

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 .

Question: In a crystal, the electric field of neighbouring ions perturbs the energy levels of an atom. As a crude model, imagine that a hydrogen atom is surrounded by three pairs of point charges, as shown in Figure 6.15. (Spin is irrelevant to this problem, so ignore it.)

(a) Assuming that rd1,rd2,rd3show that

H'=V0+3(β1x2+β2y2+β3z2)-(β1+β2+β3)r2

where

βi-e4πε0qidi3,andV0=2(β1d12+β2d22+β3d32)

(b) Find the lowest-order correction to the ground state energy.

(c) Calculate the first-order corrections to the energy of the first excited states Into how many levels does this four-fold degenerate system split,

(i) in the case of cubic symmetryβ1=β2=β3;, (ii) in the case of tetragonal symmetryβ1=β2β3;, (iii) in the general case of orthorhombic symmetry (all three different)?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free