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History 181B: Modern Physics
Class 27 (3/31/03)
Making use of quantum mechanics
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| Navigation |
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| Outline |
Moving towards the many-body problem
A new quantum number and Pauli's exclusion principle
Spin, a (sort of) intuitive picture
Counting indistinguishable particles: Quantum statistics
Fermi-Dirac (half-integral
spin)
Bose-Einstein (integral
spin)
Consequences, including the many-body problem
Putting QM to work on the structure of matter
Quantum chemistry and chemical physics
Explaining the chemical bond: The hydrogen molecule
(H2)
The sociology of a border domain
Reducing chemistry to physics? |
| Names
and terms |
| Primary |
Secondary |
Wolfgang Pauli (1900-1958), NP 1945
exclusion principle
spin
Enrico Fermi (1901-1954), NP 1938
Paul Dirac (1902-1984), NP 1933
Albert Einstein (1879-1955), NP 1921
Satyendra Nath Bose (1894-1974)
Fermi-Dirac statistics, Bose-Einstein statistics
fermions, bosons |
Samuel Goudsmit (1902-1978)
George Uhlenbeck (1900-1988)
angular momentum
spin-statistics theorem
Walter Heitler (1904-1981)
Fritz London (1900-1954)
resonance |
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| Assignment |
Wolfgang Pauli, "Exclusion Principle and Quantum
Mechanics" (1946), in Nobel Lectures: Physics, 1942-1962 (Amsterdam:
Elsevier, 1964), 27-42.
This is hard and will draw on your knowledge of chemistry.
Read pp. 27-36. You can read the rest if you like quantum field theory.
When Pauli came up with his "two-valuedness not
describable classically," what problems were concerning him: abstract theory
or practical spectroscopy? Since you probably can't follow those problems,
what would you need in order to understand what he was doing?
What did he call the exclusion principle?
At the start, could Pauli give a deep meaning to
this "two-valuedness" or a logical reason for the exclusion principle?
What did it take before they were better understood?
On p. 33, what are examples of particles in the
antisymmetrical class (Fermi-Dirac)? In symmetrical class (Bose-Einstein)?
What do these classes have to do with spin? |
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Copyright © Cathryn Carson 2003 |