| # The Miller Harmonic Method (MHM) — Technical Overview |
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| This document explains the method implemented in `batterymhm/`. The method is |
| **patent pending**; this description is provided for understanding and |
| reproduction under the repository's CC BY-NC 4.0 license. |
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| --- |
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| ## 1. The harmonic digit space and the fold map |
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| MHM works in a finite digit space **D = {1, 2, …, 9}**. Any integer is projected |
| into D by the **fold map**: |
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| ``` |
| HIN(k) = 1 + ((k − 1) mod 9) |
| ``` |
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| `HIN` stands for *Harmonic Identity Number*. In code this is `f9` (general) and |
| `hin` (applied to an atomic number Z). Two integers that differ by a multiple of |
| 9 share a harmonic class. Real-valued measurements (capacity, voltage, |
| temperature) are first quantised into 9 bins (`seq_to_harmonics`) so they, too, |
| live in D. |
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| ## 2. The binary operations |
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| Two complementary operations act on D, each folded back into D: |
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| | Operation | Symbol | Definition | Role | |
| |---|---|---|---| |
| | Creative addition | `⊕` | `f9(a + b + 1)` | recombination / creative synthesis | |
| | Growth product | `⊗` | `f9(a·b + 1)` | growth / energy exchange | |
| | Energy addition | `⊕_E` | `f9(a + b + 1 + tier)` | shell-tiered energy coupling | |
| | Miller subtraction | `⊖` | `f9(a − b + 9)` | directed harmonic difference | |
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| These are the building blocks for the histograms and the calculus below. (Note: |
| `⊕` and `⊖` are *not* exact inverses — the `+1` in creative addition is |
| deliberate and gives the algebra its asymmetry.) |
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| ## 3. The Chi compatibility matrix |
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| The heart of the method is a fixed **9×9 Chi matrix** `Χ[i, j] ∈ (0, 1]` |
| (`batterymhm/atomic.py`). `Χ[i, j]` is the harmonic *compatibility* (resonance) |
| between classes `i` and `j`. It is symmetric with a unit diagonal. |
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| The nine classes split into two physical channels: |
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| - **Matter** — classes 1–8, scored on the 8×8 sub-matrix `CHI_MATTER_8x8`. |
| - **Energy** — class 9, the "energy pole," scored on a separate 9-vector |
| `CHI_ENERGY_9`. |
| - **Tesla nodes** — classes {3, 6, 9} are energy-focusing; they get their own |
| network features. |
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| This matter/energy split lets crystal-structure models score matter–matter |
| bonding and the energy-pole contribution on distinct geometries. |
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| ## 4. The Miller sequence and shell levels |
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| The **Miller sequence** is a Fibonacci-like sequence with seed `[1, 1, 3]`: |
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| ``` |
| 1, 1, 3, 4, 7, 11, 18, 29, 47, 76, … |
| ``` |
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| Its positions group into **shell levels** (level 1 = positions 1–3, level 2 = |
| 4–12, level 3 = 13–39, …), each level three times larger than the last. These |
| levels provide a *physically meaningful sampling grid*: for a battery, level-1 |
| positions correspond to the first few cycles (the "initialization signature"), |
| and later levels to the long-term aging trajectory. The sequence and its |
| class trajectory (via **CMR**, repeated creative-addition reduction) are turned |
| into features. |
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| ## 5. Embeddings |
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| Two embeddings bridge the discrete digit space to continuous math: |
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| - **χ-embedding**: `χ(a) = (a + 1) mod 9` → an index in ℤ₉ (bridge to calculus). |
| - **φ-embedding**: `φ(d) = sin(πd / 9)` → a real number (bridge to geometry). |
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| ## 6. Miller calculus |
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| Operating on a harmonic sequence, MHM defines discrete differential operators |
| (`batterymhm/calculus.py`): |
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| - **velocity** — mean first-order Miller difference, |
| - **acceleration** — mean second-order difference, |
| - **integral** — cumulative creative addition, |
| - **curvature** — curvature `κ = |y''| / (1 + y'²)^{3/2}` of the φ-embedded |
| curve, which spikes at the onset of capacity-fade degradation (the aging |
| "knee"). |
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| Evaluated at multiple window scales, these capture multi-scale degradation |
| dynamics. |
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| ## 7. The descriptor (557 features) |
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| `mhm_full_features(hins)` returns a fixed **557-dimensional** vector |
| (`batterymhm/features.py`): |
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| | Group | # | What it encodes | |
| |---|---:|---| |
| | Chi9 full histogram | 81 | distance-weighted 9×9 compatibility | |
| | Chi9 count histogram | 81 | unweighted pair counts | |
| | HIN transition matrix | 81 | Markov ordering of the sequence | |
| | Growth-product histogram | 81 | `⊗` energy-exchange character | |
| | Energy-addition histograms (2 tiers) | 162 | `⊕_E` shell-coupled resonance | |
| | Miller-level breakdown | 27 | class occupancy per shell level | |
| | Tesla-network features | 9 | {3,6,9} focusing nodes and bridges | |
| | Multi-scale Miller calculus | 12 | velocity/accel/curvature/integral × 3 scales | |
| | Creative-addition chains | 15 | cumulative `⊕` chain statistics | |
| | CMR multi-point | 5 | reductions at 5 truncations | |
| | HIN / GP / EA entropy | 3 | diversity of harmonic interactions | |
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| For crystals, `mhm_matter8_neighbor_histograms` and `mhm_neighbor_histograms` |
| build the descriptor from the actual neighbour-pair list `(HIN_a, HIN_b, dist)`, |
| so every feature is physically grounded. |
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| ## 8. The model |
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| The descriptor feeds `MHMEnsemble` (`batterymhm/ensemble.py`): |
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| - **ExtraTrees** (600 trees) + **XGBoost** (400 trees), blended 0.75 / 0.25, |
| - with an optional **Ridge** out-of-fold stacking meta-learner, |
| - all seeds fixed at 42 for reproducibility. |
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| The ensemble is deliberately light and CPU-only; the harmonic descriptor does |
| the heavy lifting. |
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| ## 9. Two battery applications |
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| **Cell state-of-health.** Quantise an early-cycle capacity curve into HINs → |
| compute the 557-feature descriptor → predict SOH / remaining useful life. On the |
| MIT–Stanford–TRI dataset this reaches MAE 0.0114 (5-fold CV, 30% window), #1 on |
| that benchmark. |
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| **Crystal formation energy.** Fold each crystallographic site to a HIN by atomic |
| number → score neighbour pairs through the 8×8 matter matrix + HIN-9 energy |
| channel → predict formation energy. On Matbench `mp_e_form` this reaches MAE |
| 0.1513 eV/atom — better than the classic RF baseline, below modern GNNs (an |
| honest, documented limitation). |
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| --- |
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| *The fold map, the operations, the Chi matrix, the Miller sequence, and the |
| multi-scale aggregation are the subject of pending patent applications by |
| William T. L. Miller.* |
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