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.

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

(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.

Consider the isotropic three-dimensional harmonic oscillator (Problem 4.38). Discuss the effect (in first order) of the perturbation H'=λx2yz

(for some constant λ) on

(a) the ground state

(b) the (triply degenerate) first excited state. Hint: Use the answers to Problems 2.12and 3.33

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.

Consider the (eight) n=2states, |2ljmj. Find the energy of each state, under weak-field Zeeman splitting, and construct a diagram like Figure 6.11 to show how the energies evolve asBext increases. Label each line clearly, and indicate its slope.

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