The cube's Cayley-graph distance distribution is a striking diagram: nearly all 4.3 × 10¹⁹ states land at d = 18 or 19, while only 4.9 × 10⁸ states sit at d = 20. This distribution is exactly what the God's-number-20 proof produced.
Vertical axis is log₁₀(count). A few features to notice:
| Metric | Generators | Diameter | Random avg | Bound proof |
|---|---|---|---|---|
| HTM (half-turn) | 18 | 20 | ~18 | 2010 Rokicki et al. |
| QTM (quarter-turn) | 12 | 26 | ~22 | 2014 Rokicki & Kociemba |
| STM (slice) | 27 | ≤ 20 (unproven) | ~17 | partial enumerations |
Four states were once known as "the furthest": superflip (all edges flipped; Reid 1995 proved it requires 20 HTM), and superflip composed with the 4-spot or 6-spot patterns. After 2010, the full census reveals 4.9 × 10⁸ states at exactly distance 20.
The table below gives exact counts for d = 0…15 (full enumeration, Kociemba 2013) and the established counts for d = 16…20 (symmetry-reduced proofs after Rokicki et al. 2014). The column totals to |G| = 43,252,003,274,489,856,000.
| d | states at d | fraction of |G| | ratio |
|---|---|---|---|
| 0 | 1 | ~0 | — |
| 1 | 18 | ~0 | 18.0× |
| 2 | 243 | ~0 | 13.5× |
| 3 | 3,240 | ~0 | 13.3× |
| 4 | 43,239 | ~0 | 13.3× |
| 5 | 574,908 | ~0 | 13.3× |
| 6 | 7,618,438 | ~0 | 13.3× |
| 7 | 100,803,036 | ~0 | 13.2× |
| 8 | 1,332,343,288 | 3.1 × 10-11 | 13.2× |
| 9 | 17,596,479,795 | 4.1 × 10-10 | 13.2× |
| 10 | 232,248,063,316 | 5.4 × 10-9 | 13.2× |
| 11 | 3,063,288,809,012 | 7.1 × 10-8 | 13.2× |
| 12 | 40,374,425,656,248 | 9.3 × 10-7 | 13.2× |
| 13 | 531,653,418,284,628 | 1.2 × 10-5 | 13.2× |
| 14 | 6,989,320,578,825,358 | 1.6 × 10-4 | 13.1× |
| 15 | 91,365,146,187,124,313 | 2.1 × 10-3 | 13.1× |
| 16 | ≈ 1.10 × 1018 | 2.5% | 12.0× |
| 17 | ≈ 1.22 × 1019 | 28.3% | 11.1× |
| 18 | ≈ 2.98 × 1019 | 68.9% | 2.4× |
| 19 | ≈ 1.50 × 1018 | 3.5% | 0.05× |
| 20 | 490,000,000 | 1.1 × 10-11 | 3.3 × 10-10× |
| 21+ | 0 | 0 | — |
| Σ | 4.325 × 1019 | 100% | = |G| |
The "ratio" column shows the geometric structure of the Cayley graph: from d = 1 to d = 15, each shell grows by ~13.2× (well below 18, because moves like overlap and reduce the effective branching factor). Then between d = 16…18, growth saturates dramatically — 97% of G's elements cluster in shells 17 and 18. d = 19 already drops to 3.5%; d = 20 is nearly empty (only 4.9 × 108). This is the canonical "ball explosion then boundary collapse" shape of finite Cayley graphs.
For any group G with generating set S, the ball growth function isthe total state count within radius r. For the finite cube group, B(r) saturates at |G| for r ≥ 20. For infinite groups (free groups, hyperbolic groups), the asymptotic growth of B(r) reveals a group's "geometric dimension."