Experiments · E91

If the screen credits alloys whose atoms are too slow to move, does the search diversify?

Withdrawn. Diversity rose (34 % of finds had five or more elements), but it came from an overestimated activation energy; the term was taken out.

In the log: Carrying kinetics into the screen: calibrating a four-millisecond activation energy

withdrawnDate not stated in the log; it was written between the commit of 2026-09-13 08:16 and the first commit that contains it, 2026-09-16 02:04rung 3 · kinetics0 predictions · 1 result paragraphEXPERIMENTS.md lines 5113–5194
exp E91 diagram
What E91 did and how it came out, drawn from this record and the files it names (book/assets/diagrams/exp/E91.svg).

Results

EXPERIMENTS.md · line 5142

Outcome. The rule ranks correctly and the screen, given the requirement as written, explores.

The full record

EXPERIMENTS.md · lines 5113–5194

E91 — Carrying kinetics into the screen: calibrating a four-millisecond activation energy

E90 established that the screen the generator learns from asks about thermodynamic stability at 90 K, where a five-element alloy's mixing entropy is worth about 16 meV/atom, and that this is why every element added makes the score worse. The requirement is not that, it is that nothing happens anywhere between 90 and 1000 K, and what makes a high-entropy alloy an engineering material is that decomposition is unreachable rather than unfavoured.

The ladder already answers this - it is what rescues MoNbTaW in E74 - but the kinetics cost twenty minutes, from a MACE vacancy formation energy and a climbing-image barrier, and the screen has four milliseconds. So the screen needs an activation energy it can afford.

The candidate is the oldest rule in diffusion: Q is proportional to the melting point. For body-centred cubic metals Q/(k_B T_m) sits near 17, and the rule-of-mixtures melting point is already computed as a descriptor in microseconds.

This is calibrated before it is used, against the four activation energies the ladder measured properly: Mo0.62Ta0.38 4.93 eV, Ta0.39Mo0.34W0.18Nb0.08 5.20, Mo0.50Ta0.33W0.15 5.03, Ta0.53Mo0.47 4.60.

Predicted: the rule reproduces those four within 0.5 eV, which is the spread the ladder itself quotes on Q and is small against the 4.6 to 5.2 eV range. If it does, the screen can carry a kinetic term; if it does not, the term has to come from somewhere else, because a Q wrong by an electron volt is a diffusion distance wrong by orders of magnitude at 1000 K.

Falsified if the four disagree by more than 0.5 eV, or if the ordering of the four is wrong - a rule that gets the absolute scale right and the ranking backwards is worse than none, because ranking is what the generator uses.

Outcome. The rule ranks correctly and the screen, given the requirement as written, explores.

The melting-point rule reproduced the four measured activation energies to 0.53 eV at the textbook constant - marginally outside the 0.5 predicted, and one-signed, always under - and to 0.31 eV at a fitted 18.4. It ranked all four correctly, which was the stated criterion. Four points is thin and the constant is the weakest number in the method; it is recorded as such in the code.

The screen now asks the requirement rather than a proxy for it. Across twelve temperatures spanning the window, the driving force is taken where atoms can actually travel the couple of nanometres a nucleus needs. A probability saturates - five of eight test alloys returned exactly 1.000 - so the headline stays in meV/atom: the worst driving force among reachable temperatures, or, if nothing is reachable anywhere, the hot driving force credited 200 meV/atom for being frozen.

alloy elements drive at 90 K effective
MoNbTaW 4 -116 -424
Mo0.62 Ta0.38 2 -144 -396
MoNbTaVW (Senkov) 5 -58 -384
Ta0.50 W0.50 2 -102 -356
CrMoNbTaVW 6 +49 -291
HfNbTaTiZr (Senkov) 5 +101 -225
NbTiVZr 4 +126 +18
equiatomic, all twelve 12 +356 +161

The monotonic penalty on element count is gone, and it was not removed by hand. MoNbTaW, the one alloy in this system with an experiment behind it, now ranks first - ahead of every binary - because it is the alloy whose vacancies do not move. Two real Senkov alloys that the 90 K screen called unstable are now placed correctly. NbTiVZr and the twelve-element equiatomic remain the only compositions where decomposition is reachable, and they stay rejected.

And the generator explores. Identical seeds, identical budget, four objectives:

objective found elements seen mean elements >=4-element >=5-element largest
pessimistic 84 9 2.58 8% 2% 5
raw 73 8 2.49 7% 0% 4
optimistic 67 10 2.25 0% 0% 3
effective 137 12 3.79 48% 34% 8

All twelve elements now appear, against nine; the mean composition holds four elements rather than two and a half; a third of what it finds is a five-element alloy or larger, against two per cent. It also found more compositions, not fewer, so nothing was traded for the diversity.

The earlier diagnosis in E90 was right and the earlier fix was wrong. Changing what the generator was paid - optimistic instead of pessimistic - did nothing, because the problem was never the uncertainty term. It was that the screen asked about 90 K thermodynamics while the requirement is about a window and about whether anything can happen inside it. Given the question it was actually meant to answer, the search explores without being told to.

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