Finite Wells & Quantization
Bound states from boundary conditions; discrete allowed energies; nonzero probability structure inside the well.
Common misconception: probability is not flat just because the classical region looks "allowed."
Core facts
- Name the objects precisely — symbols before slogans.
- State the governing identity or update rule for this lesson.
- Compute one tiny example by hand before touching software.
- Track what assumption would break the formula.
- Rephrase the result in one sentence a teammate could check.
Why this matters
This chapter exists so you can move numbers, not just recognize vocabulary. If you cannot reproduce the worked examples with paper closed after one pass, treat the interactive lab as diagnosis, not entertainment.
Derivation sketch
Write the definition, apply the main theorem or algorithm step, then specialize to a two- or three-dimensional toy case. Keep units / probability normalization visible. The interactive at the end should match your hand calculation within noise.
Worked example A
Take the simplest nontrivial parameters from the definitions above. Compute the primary quantity twice: once symbolically, once numerically. Compare.
Worked example B
Change one assumption (rate↔mean, train↔test, real↔risk-neutral, classical↔quantum). Predict the direction of change before recalculating.
Pitfalls
- Confusing a definition with a theorem that needs hypotheses.
- Using a formula outside its domain (logs of logs, probabilities outside , unstable generators).
- Treating a simulation path as proof.
- Skipping the checkpoint and jumping to the lab.
Checkpoint
- Restate the main identity of without looking.