Atomic Physics - Modern Physics - Lecture Slides, Slides of Physics

A great and very useful lecture on Modern Physics. These lecture slides include: Atomic Physics, Atomic Structure and the Periodic Table, Pauli Exclusion Principle, Atomic Structure, Lanthanides, Actinides, Angular Momentum, Lscoupling, Anomalous Zeeman Effect

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2013/2014

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8.1 Atomic Structure and the Periodic Table
8.2 Total Angular Momentum
8.3 Anomalous Zeeman Effect
Atomic Physics
What distinguished Mendeleev was not only genius, but a
passion for the elements. They became his personal friends; he
knew every quirk and detail of their behavior.
- J. Bronowski
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 8.1 Atomic Structure and the Periodic Table

 8.2 Total Angular Momentum

 8.3 Anomalous Zeeman Effect

Atomic Physics

What distinguished Mendeleev was not only genius, but a passion for the elements. They became his personal friends; he knew every quirk and detail of their behavior.

  • J. Bronowski

8.1: Atomic Structure and the Periodic Table

 What would happen if there are more than one electron? a nucleus with charge +2e attracting two electrons. the two electrons repelling one another.  Can not solve problems exactly with the Schrödinger equation because of the complex potential interactions.  Can understand experimental results without computing the wave functions of many-electron atoms by applying the boundary conditions and selection rules.

Atomic Structure

Hydrogen : ( n , ℓ, m ℓ, ms ) = (1, 0, 0, ±½) in ground state.  In the absence of a magnetic field, the state ms = ½ is degenerate with the ms = −½ state. Helium : (1, 0, 0, ½) for the first electron. (1, 0, 0, −½) for the second electron.  Electrons have antialigned ( ms = +½ and ms = −½) spins as being paired. Supports Pauli exclusion principle.  The principle quantum number also has letter codes.  n = 1 2 3 4...  Letter = K L M N…  n = shells (eg: K shell, L shell, etc.)  n ℓ = subshells (eg: 1 s , 2 p , 3 d ) Electrons for H and He atoms are in the K shell. H: 1 s^2 He: 1 s^1 or 1 s

Atomic Structure

How many electrons may be in each subshell? Recall: ℓ = 0 1 2 3 4 5 … letter = s p d f g h … ℓ = 0, ( s state) can have two electrons. ℓ = 1, ( p state) can have six electrons, and so on. The lower ℓ values have more elliptical orbits than the higher ℓ values. Electrons with higher ℓ values are more shielded from the nuclear charge. Electrons lie higher in energy than those with lower ℓ values. 4 s fills before 3 d. Total For each m ℓ: two values of ms 2 For each ℓ: (2ℓ + 1) values of m ℓ 2(2ℓ + 1)

Groups and Periods

Groups :  Vertical columns.  Same number of electrons in an ℓ orbit.  Can form similar chemical bonds. Periods :  Horizontal rows.  Correspond to filling of the subshells.  Some properties of elements are compared by the ionization energies of elements and atomic radii.

The Periodic Table

Inert Gases :  Last group of the periodic table  Closed p subshell except helium  Zero net spin and large ionization energy  Their atoms interact weakly with each other Alkalis :  Single s electron outside an inner core  Easily form positive ions with a charge +1e  Lowest ionization energies  Electrical conductivity is relatively good Alkaline Earths :  Two s electrons in outer subshell  Largest atomic radii  High electrical conductivity

The Periodic Table

Lanthanides ( rare earths ) :  Have the outside 6 s 2 subshell completed  As occurs in the 3 d subshell, the electrons in the 4 f subshell have unpaired electrons that align themselves  The large orbital angular momentum contributes to the large ferromagnetic effects Actinides :  Inner subshells are being filled while the 7 s 2 subshell is complete  Difficult to obtain chemical data because they are all radioactive  Have longer half-lives

8.2: Total Angular Momentum

L , Lz , S , SzJ and Jz are quantized. Orbital angular momentum Spin angular momentum Total angular momentum

Spin-Orbit Coupling

 An effect of the spins of the electron and the orbital angular momentum interaction is called spin-orbit coupling.  is the magnetic field due to the proton.

where cos a is the angle between.

  • The dipole potential energy.
  • The spin magnetic moment  -.

Total Angular Momentum

No external magnetic field :  Only Jz can be known because the uncertainty principle forbids Jx or J y from being known at the same time as J z

Total Angular Momentum

 Now the selection rules for a single-electron atom become  Δ n = anything Δℓ = ± 1  Δ mj = 0, ± 1 Δ j = 0, ± 1  Hydrogen energy-level diagram for n = 2 and n = 3 with the spin- orbit splitting.

Many-Electron Atoms

Hund’s rules :

  1. The total spin angular momentum S should be maximized to the extent possible without violating the Pauli exclusion principle.
  2. Insofar as rule 1 is not violated, L should also be maximized.
  3. For atoms having subshells less than half full, J should be minimized.  For labeled two-electron atom  There are LS coupling and jj coupling to combine four angular momenta J.

LS Coupling

 The notation for a single-electron atom becomes n^2 S +1^ LJ  The letters and numbers are called spectroscopic symbols.  There are singlet states ( S = 0) and triplet states ( S = 1) for two electrons.

LS Coupling

 There are separated energy levels according to whether they are S = 0 or 1.  Allowed transitions must have Δ S = 0.  No allowed ( forbidden ) transitions are possible between singlet and triplet states with much lower probability.