Why an orbital-filling toy model can land on Fibonacci numbers.
Aufbau gives us an ordered list of increasingly costly one-electron states. Fibonacci enters only after we add a separate combinatorial rule: among a line of ordered positions, no two occupied positions may sit next to one another.
Aufbau: lower-energy states are filled before higher-energy ones
In the familiar atomic picture, electrons are placed into low-energy orbitals first, subject also to Pauli and Hund. The common Madelung \(n+\ell\) order is a useful mnemonic, not an exact universal energy theorem: orbital energies depend on the atom and on occupancy, and well-known configuration exceptions occur.
Turn an ordered list into 0/1 slots
Let \(x_i=1\) mean position \(i\) is selected and \(x_i=0\) mean it is not.
Now impose the extra rule
so consecutive 1s are forbidden.
Choose N
Exactly k occupied positions
Choose k non-adjacent slots
Compress away the mandatory gaps between occupied sites.
Sum over k
The largest possible k is \(\lceil N/2\rceil\).
Fibonacci identity
Convention: \(F_0=0,\ F_1=1\).
| k occupied | count | formula |
|---|---|---|
| Total | ||
The coefficients lie on a shallow diagonal
For fixed \(N\), the coefficients \(\binom{N-k+1}{k}\) are entries of Pascal’s triangle. Their shallow-diagonal sum is \(F_{N+2}\).
The recurrence is even simpler
Let \(A_N\) be the number of legal strings of length \(N\). If the first slot is 0, there are \(A_{N-1}\) possibilities. If it is 1, the next slot must be 0, leaving \(A_{N-2}\) possibilities.
Hence \(A_N=F_{N+2}\).
Physics retained
- an approximate energy ordering of atomic orbitals
- Pauli and Hund constrain real electron filling
- Aufbau organizes low-to-high energy occupation
Extra combinatorial rule
- reduce each ordered position to a binary choice
- forbid adjacent occupied positions
- that nearest-neighbour exclusion creates Fibonacci counting