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Magnetic

Bohr magneton

(g factor) determined by details of charge distribution

( e.g. ) (QED corrections for electron) 7-31. Assuming the electron to be a classical particle, a sphere of radius 10-15 m and a uniform mass , use the magnitude of the | S | = [s (s+1)]1/2 ħ=(3/4)1/2 ħ to compute the speed of rotation at the electron’s equator. How does your result compare with the ? Magnetic moment Stern-Gerlach experiment

Inhomogeneous magnetic Stern-Gerlach experiment

Inhomogeneous Stern-Gerlach experiment

Inhomogeneous magnetic field

Classical picture – continuum of possible orientations – 2l +1 deflections ? Stern-Gerlach experiment Total Angular Momentum

total angular momentum

or

If J1 is one angular momentum (orbital, spin, or a combination) and J2 is another, the resulting total angular momentum J = J1 + J2 has the value [ j ( j + 1)]1/2 ħ for its magnitude, where j can be any of the values j1 + j2, j1 + j2 - 1, . . . , | j1 - j2 | 7-34. (a) The angular momentum of the yttrium in the is characterized by the quantum number j = 3/2. How many lines would you expect to see if you could do a Stern-Gerlach experiment with yttrium ? (b) How many lines would you expect to see if the beam consisted of atoms with zero spin, but l= 1? a)

b) 7-37. A atom is in the 3d state (n = 3, l = 2). (a) What are the possible values of j? (b) What are the possible values of the magnitude of the total angular momentum? (c) What are the possible z components of the total angular momentum?

a) b) c) Spectroscopic Notation

Single electron s p d f g h l 0 1 2 3 4 5

K L M N O n 1 2 3 4 5

Atomic state total spin total orbital angular momentum

n total angular momentum

Hydrogen ground state Identical Particles in Quantum Mechanics

Non-interacting particles

e.g. Identical Particles in Quantum Mechanics

Symmetric wavefunctions –bosons (e.g photons)

Antisymmetric wavefunctions –fermions (e.g )

Symmetric wavefunctions –bosons (e.g photons)

Antisymmetric wavefunctions –fermions (e.g electrons) Pauli Exclusion Principle

No more than one electron may occupy a given quantum state specified by a particular set of single- particle quantum numbers n, l, ml ms. Ground State of Atoms

He (Z=2)

1s2 – ground state

(more accurate calculations to be used)

He+

Energy needed to remove the first electron (first ionization) potential is 24.4 eV Ground State of Atoms l=0 m=0 ms=±1/2 2 electrons l=1 m=-1,0,1 ms=±1/2 6 electrons l=2 m=-2,-1,0,1,2 ms=±1/2 10 electrons ground state last electron H : 1s1 n=1, l=0 He: 1s2 (filled shell n=1) n=1, l=0

Li: 1s2 2s1 n=2, l=0 Be: 1s2 2s2 n=2, l=0 B : 1s2 2s2 2p1 n=2, l=1 C : 1s2 2s2 2p2 n=2, l=1 N: 1s2 2s2 2p3 n=2, l=1 O: 1s2 2s2 2p4 n=2, l=1 F: 1s2 2s2 2p5 n=2, l=1 Ne: 1s2 2s2 2p6 (filled shell n=2) n=2, l=1 Ground State of Atoms

ground state last electron Na: 1s2 2s2 2p6 3s1 n=3, l=0 Mg: 1s2 2s2 2p6 3s2 n=3, l=0 Al: 1s2 2s2 2p6 3s2 3p1 n=3, l=1 Si : 1s2 2s2 2p6 3s2 3p2 n=3, l=1 P: 1s2 2s2 2p6 3s2 3p3 n=3, l=1 S: 1s2 2s2 2p6 3s2 3p4 n=3, l=1 Cl: 1s2 2s2 2p6 3s2 3p5 n=3, l=1 Ar: 1s2 2s2 2p6 3s2 3p6 n=3, l=1

K: 1s2 2s2 2p6 3s2 3p6 3d1 n=3, l=2 K: 1s2 2s2 2p6 3s2 3p6 4s1 n=4, l=0 Ground State of Atoms

2p state is almost always outside 1s electrons - sees the effective charge Zeff =+1 2s state penetrates the shielding of 1s electrons more positive charge –lower for 2s Ground State of Atoms

Li: 1s2 2s1

Greater l smaller involves penetration effect and large

The large penetration effect makes the energy 4s lower than 3d. 7-46. Write the ground-state of (a) carbon, (b) , and (c) argon.

C : 1s2 2s2 2p2

O: 1s2 2s2 2p4

Ar: 1s2 2s2 2p6 3s2 3p6 7-50. If the 3s electron in sodium did not penetrate the inner core, its energy would be -13.6 eV/32 = -1.51 eV. Because it does penetrate, it sees a higher effective Z and its energy is lower. Use the measured ionization potential of 5.14 V to calculate Zeff for the 3s electron in sodium. 2 2 7-41. The Lamb shift energy difference between the 2 S1/2 and 2 P1/2 levels in atomic hydrogen is 4.372 x 10-6 eV. (a) What is the frequency of the photon emitted in this transition? (b) What is the photon’s wavelength? (c) In what part of the electromagnetic spectrum does this transition lie? a) b)