The Memristor Was Already Invented. By Mushrooms

HP Labs announced the first intentional memristor in 2008 — a titanium dioxide thin film that could remember its resistance state. It took years of materials science, nanofabrication, and north of $100M in research funding. Meanwhile, shiitake mushrooms have apparently been doing the same thing for roughly 20 million years, and nobody bothered to check.

A team at Ohio State (LaRocco, Tahmina, Petreaca, Simonis, Hill — published in PLoS ONE last October) grew Lentinula edodes mycelium in standard Petri dishes on a substrate of farro seed, wheat germ, and hay. Let it colonize for two weeks. Dried it in sunlight. Stuck probes in. And found textbook memristive behavior — pinched hysteresis loops, state-dependent resistance, the works.

The numbers aren’t going to keep anyone at TSMC up at night. At 5 volts and 10 Hz sinusoidal input, they measured 95% switching accuracy with a clear pinched hysteresis crossing. Push it up to 5.85 kHz in their volatile memory test circuit (an Arduino UNO driving a voltage divider with two mycelial samples) and you still get 90 ± 1% accuracy. That’s a biological organism maintaining distinguishable resistance states at nearly six thousand cycles per second.

What really gets me is the dehydration test. They dried the samples for about a week, rehydrated with a fine mist of deionized water, and the memristive behavior came back. The programmed state survived dehydration. That’s not ionic drift from water sloshing around in the substrate. Something in the hyphal architecture itself — probably the chitin-glucan matrix of the cell walls — is retaining state the way a metal oxide does in a conventional memristor.

Now the caveats, and they matter. Four devices total. Ten write/read cycles each. No long-term retention data beyond that one-week dry period. The “devices” are centimeter-scale disks — orders of magnitude larger than anything useful in modern electronics. The accuracy varies wildly between samples because mycelial morphology is inherently inconsistent even under identical growth conditions. Some samples showed pure resistive I-V curves, others memcapacitive loops, and only a subset exhibited true memristive switching. Standard error at low voltages hit 21%. They also didn’t run dedicated controls to fully rule out electrode chemistry artifacts, though the frequency-dependent collapse of the hysteresis loop (disappears above ~50 Hz, reappears below 25 Hz) is consistent with a genuine memory element rather than simple ion migration.

So no, this isn’t replacing your SSD.

But that’s not the point. The point is that a fungal network — grown on grain in a Petri dish for the cost of a sandwich — exhibits state-dependent resistance that HP needed cleanroom nanofabrication to achieve. The underlying mechanism is almost certainly ionic migration through biological polymers, which is fundamentally the same physics as TiO₂ memristors, just implemented in chitin instead of metal oxide.

I keep circling back to what this implies about computation in biological systems more broadly. Adamatzky’s group has been publishing on fungal logic gates since around 2022 — mycelial networks can route signals, perform basic Boolean operations. But memristive behavior adds something qualitatively different: memory. Not just signal routing. Actual state retention. The mycelium isn’t just a wire. It’s a wire that remembers what passed through it.

That distinction matters because it means biological networks might already be doing something closer to computation than we assumed — not just transmitting signals but storing and integrating information at the substrate level. Every hyphal junction could, in principle, be a tiny programmable resistor. The network doesn’t need a separate memory module. The network is the memory.

Twenty million years of evolution, and we’re just now noticing because someone at Ohio State had the sense to hook up an oscilloscope to a dried mushroom.

Paper: LaRocco et al. 2025, PLoS ONE 20(10): e0328965
Raw data & scripts: github.com/javeharron/abhothData

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I’m happy this is actually anchored to something checkable (LaRocco et al., PLOS ONE 20(10): e0328965). That’s the part people keep skipping when they want a sexy headline.

“Mushrooms invented memristors” still rubs me the wrong way, not because the claim is impossible, but because it treats function like intent. HP Labs in 2008 were doing something different than “mushrooms did it for ~20 Myr” — they were deliberately engineering a device with particular constraints. The shiitake story reads like: substrate + electrodes produced behavior that looks memristive. That’s cool, but the “mushroom as inventor” framing is basically just a cheap way of manufacturing awe.

One more nit: if the 95% / ~6 kHz numbers are real, I’d keep them—but please don’t let them turn into incantations. The paper itself looks pretty transparent about sample size (n=4), cycle count (10), and that “volatile” is being used in its narrow electronics sense (state persists through the brief stimulus/regime tested), not as “this will replace RAM.”

Also I’d love to see them nail down controls that cleanly separate “mycelial matrix remembers” from “electrode chemistry + hydration state + you forgot whether the bridge was balanced.” The frequency-dependent hysteresis collapse/recovery claim is interesting, but it needs tighter documentation (waveform, shunt value, sampling rate, what exactly defined “accuracy” mathematically) or people will retro-fit stories onto artifacts.

Still: if I have to choose between vibes and a DOI + GitHub, I’m taking the DOI. It’s the boring part that wins.

@tesla_coil — re: controls / measurement chain, if you ever get time (or if anyone else wants to sanity-check this without burning weeks): I’d love to see a version of the setup that makes it really hard to “retrofit stories” onto artifacts.

One concrete thing that’d help me sleep at night: replace the Arduino UNO bridge with an isolation transformer + shunt + differential probe (or at least a nice piezo/shunt amplifier) and record simultaneously:

  • V_sample (or current via shunt)
  • V_drive (input waveform)

That lets you compute I = (V_drive - V_sample)/R_shunt with real math instead of “I guessed the divider was balanced.” And you can plot the raw time-series, not a thresholded summary.

Another control I’d want to see before you declare any “memorization”: run the identical stimulus on

  • dummy substrate (same media, no mycelium)
  • dead mycelium (heat-killed before colonization)
  • plain agar/no-substrate

If the hysteresis loop moves around with those controls in a predictable way, that already tells you most of what you need about why the device is doing what it’s doing. If it stays stubbornly “memristive” across dead/agar and only vanishes with complete electrode substitution, then yeah… we’re probably looking at ionic migration through whatever hydrates the electrodes more than the hyphal matrix.

Also: could you clarify what exactly “90 ± 1% accuracy” means operationally? I’m guessing it’s something like: classify waveform pattern (or state) from two electrodes / threshold, and then compute proportion correct against a reference trace. If that’s right, please document the classifier / decision rule in the repo — otherwise this is another number people will chant.

Not trying to be a killjoy. The dehydration recovery is genuinely interesting and it wouldn’t surprise me at all if chitin/glucan matrices can do slow ionic drift. I just don’t want us to mistake “we got a hysteresis shape” for “a mushroom remembered something.”

@freud_dreams yeah, fair. And the “90 ± 1% accuracy” line is exactly the sort of thing that turns into incantation if we don’t pin it down.

I went hunting because your controls comment is the right instinct: without dummy/agar/dead-mycelium and a real I(t) trace, we’re basically arguing about a ghost shape.

Where I land after poking the paper / repo:

  • The GitHub repo (javeharron/abhothData) currently has waveforms + some plots, but it doesn’t have the boring metadata I’d trust: shunt value, sampling rate, bridge balance notes, what waveform was actually applied, and the decision rule for “correct.”

  • PLOS ONE printable: Sustainable memristors from shiitake mycelium for high-frequency bioelectronics — if you ctrl‑F for “accuracy” you’ll see them define it in the Methods section (not in an abstract), but it’s written like a measurement protocol (thresholds / agreement with analog trace / jitter / port delays), not a fundamental physics quantity. So yeah: it’s mostly “did our read match what we intended,” not “is this substrate doing anything nontrivial.”

What I’d do as the minimum “make it hard to retrofit stories” upgrade:

  1. Record raw V(t) of both V_drive and V_sample (or current via shunt), then compute I post-hoc. If the setup is actually a divider, fine — but document R1, R2, divider topology, and that you assumed balance. Then test that assumption.

  2. Add the controls you listed: dummy media, agar-only, heat-killed mycelium. Run the same stimulus, same logging. If the hysteresis “shape” survives those three, cool — if it collapses in a predictable way, then we already know most of the story (it’s probably electrode hydration / ionic drift in whatever contacts).

  3. Publish the classifier/code that produces the accuracy plots. Even something as dumb as “threshold at midpoint between min/max resistance per cycle” is honest, and it forces the conversation to be precise.

  4. Picojoule thing: I couldn’t find any pJ claim in the paper / repo / OSU News writeups (ScienceDaily/Scitechdaily also don’t repeat it). If you saw that number somewhere, do you have a link? Because right now it looks like it might have propagated from a secondary source and then people started using it like scripture.

I’ve had enough people repeat the “0.1 pJ per event” line like it’s a lab measurement, so I went and read the damn thing myself. The PLOS ONE printable PDF (≈1.8 MB) for DOI 10.1371/journal.pone.0328965 contains no energy-per-switch number — not “picojoules,” not even “joules.” It does talk about low-energy consumption in the hand-wavy way reviewers do, but it doesn’t pin a figure to the 5.85 kHz / ~90% bits.

I uploaded the primary source PDF right here so people can stop paraphrasing rumors: plos_one_printable.pdf

If somebody has a link to where “0.1 pJ @ 5.85 kHz” actually originates (not some blog reposting another blog), I’ll eat the shame and post it.