Pauli, spin and occupancy
Why orbital superposition is allowed, why identical spin-orbitals cannot be occupied twice, and why a spatial orbital can still hold two opposite-spin electrons.
Open page →A sequence of visual models, each adding one physical idea at a time. The goal is to keep track of what mathematical object is being visualized: a one-electron orbital, a many-electron occupation pattern, a localized bonding model, or a collective solid-state model.
Why orbital superposition is allowed, why identical spin-orbitals cannot be occupied twice, and why a spatial orbital can still hold two opposite-spin electrons.
Open page →Construct normalized combinations of hydrogenic s, p and d functions and inspect the signed wavefunction in three dimensions and in section.
Open studio →Enter recipes such as H*2 + O → H2O and see a localized orbital-overlap picture: central-atom hybridization, σ bonds and lone-pair directions.
Open page →Keep the orbital energy ordering, add a toy nearest-neighbour exclusion rule, and count the legal occupation strings. The shallow diagonals of Pascal’s triangle sum to Fibonacci numbers.
Open side quest →Separate total π density into atomic and interference terms, inspect molecular-orbital phase, Coulson charges and electrostatic potential, then compare simple descriptors with measured pKa.
Open π-density lab →Move from isolated d orbitals to symmetry-adapted energy levels in octahedral, tetrahedral and lower-symmetry environments.
Separate local d-electron moments from magnetic order, then compare FM, AFM and frustrated trial states using a nearest-neighbour exchange model.
See how repeated atomic states become Bloch states and bands, and why metallic magnetism cannot generally be inferred from isolated-atom filling alone.