Title: Development of the Quantum Theory
1Development of the Quantum Theory
- Progress was piecemeal, but accelerated once
physicists began to accept the idea of a
dualistic nature in light - I was compelledto assert its unambiguous
verification in spite of its unreasonablenessit
seemed to violate everything we knew about the
interference of light - - R. Millikan, 1915
- Light is a particle
- Photoelectric effect
- Compton effect
- Pair production
- Light is a wave
- Refraction
- Interference
- Diffraction
- Polarization
2Wave-Particle Duality
Louis deBroglie (1924) - If light (waves) can be
made to manifest particle (photons) behavior, why
shouldnt particles (say, electrons) manifest
wave properties?
Unstable electron orbit
Stable electron orbit
3Wave-Particle Duality
Wavelength of a particle
4Thats a bunch of crap, Dr B!...
If this is all true, why dont we see the moon
jump between allowed orbits???
Here size matters.the size of the wavelength
that is.
Wavelength of an electron
Wavelength of the moon
5Pauli and the Exclusion Principle
- Problem with Bohr model
- WHY dont electrons all go into ground state?
- WHY do electrons fill these orbital shells?
- Pauli develops exclusion principle
- Two electrons cannot occupy the same state
- That is, shells have certain number of vacancies
6Periodic Table
7The State of Quantum Theory Circa 1925
- Still only a semblance of a consistent theory
for one-electron atoms - Theory in many ways was enormously successful,
in many ways bitterly disappointing
a lamentable hodgepodge of hypotheses,
principles, theorems and computational
recipes. - Max Jammer
8Heisenbergs Matrix Mechanics
- 1925 Heisenberg develops matrix mechanics
- Differential operators correspond to physical
measurements - In matrix mathematics, these operators dont
always commute
9Heisenbergs Uncertainty Principle
- Any two operators or quantities (whose product
gives units of action) do not commute - that
is, - A x B B x A ? 0
- and cannot be simultaneously known with unlimited
precision DADB gt h Ex Dx Dp gt h - DE Dt gt h
- This is NOT a statement limiting experimental
precision, but rather a fundamental
characteristic of nature
10To measure something, you must interact with
itOn a macroscopic scale, the influence of this
interaction is negligible, but in the quantum
case it is of fundamental import Experiment
phenomena observer form one holisticnon-separa
ble systemany observation necessitates an
interference with the course of the phenomena,
and requires a final renunciation of the
classical ideal of causality and a radical
revision of our attitude towards the problem of
physical reality-Bohr
The Measurement Problem