The most famous quantum mechanical relation is the uncertainty relation, e.g. for space \(x\) and momentum \(p\)
| \begin{equation*} \Delta x \Delta p \geq \hbar \end{equation*} | (1.1) |
Pauli Principle
principally non distinguishable particles \(\Leftrightarrow\) classical particles
Fermi statistics
Bose Statistics
Tunneling
Why are atoms stable?
Quantization:
”Chemistry”: Period system of elements
sp\(^{3}\) hybridization
Spin
Band structure: Why is \(E(k)\) an adequate description of the energy of a crystal
Transport of electrons: from occupied state \(\Rightarrow\) free state
Only reasonable for Fermions following the Pauli principle!
But ”free” and ”occupied”
states within a band, sizes of band gaps, etc. classify metals, semiconductors, and insulators.
Why, in contrast, must photons be Bosons?!? (One single QM state macroscopically measurable)
What is:
Schrödinger equation, Operator, commutator, probability function,
wave function, quantum number, ......
Not discussed in this lecture
Current flow: Drift (classical forces), Diffusion (Fick’s laws, no \(E(k)\)!)
pn-junction (Poisson equation)
Devices (are temperature dependent!)
...
This are topics of Thermodynamics (mainly described classically!)
Quantum Mechanics
Are 5 Axioms: Extremely compact
information, nearly not to understand from the beginning
\(\Rightarrow\) We will need some
time to interpret the axioms
Before we will need some time to discuss the mathematics necessary for
understanding the phrases in the axioms. Operators, wave function, expectation values, measurable quantities, .....
© J. Carstensen (Quantum Mech.)