The deep dive · one of eight answers to the same experiment
Pilot Wave
“There was always a particle.”
Physics spent a century calling this theory unnecessary. It spent the century being right anyway.
In 1992 a shipping container cracked open in a Pacific storm, and 28,000 rubber ducks went overboard. For the next twenty years they kept landing — Alaska, Hawaii, eventually England — and not randomly: bunches here, nothing there, the same beaches over and over. Scientists were thrilled, because the ducks were drawing a map.
Each duck drifted alone — one dumb bit of yellow plastic riding one line of water. But the ocean it rode is a single connected thing, and the ocean knew the whole route. The ducks never did. They didn't have to.
Now shrink it.
The experiment that started all the trouble
Fire tiny particles at a wall with two slits, one at a time, with a screen behind it. One at a time matters: there's only ever one particle in flight. Common sense says each one goes through one slit or the other, and you get two piles. You don't get two piles. You get stripes — the pattern waves make when they ripple through both slits and overlap. So you put a detector at the slits to catch which one each particle uses. The stripes vanish. Two piles.
Everything on this page is one theory's answer to a single question: what, in the name of God, is going on between the gun and the screen?
Drag to orbit — two fingers on a touchscreen. Particles leave one at a time and land one at a time. The middle is deliberately not drawn — what happens there is the whole argument, and the lens is this theory's answer.
The idea
What if the particle is just... always somewhere? Pilot-wave theory says every particle has a real position at every moment, and a real wave travels with it, steering it — like a surfer riding a swell they can't see. The famous double-slit mystery stops being a mystery: the particle goes through one slit, its wave goes through both, and the wave steers the particle into the stripy pattern. No dice. No riddles. A mechanism.
What it fixes
The measurement problem, completely. A measurement just finds out where the particle already was. The moon is there when nobody looks, and so is everything else.
What it costs
The wave connects distant particles instantly — poke one here and the steering changes there, faster than light, no apology. (You still can't use it to text faster than light. Somehow that's more frustrating.) Also: nearly a century of being right on principle while nobody signs you.
The story
In 1927, at the most famous physics conference ever held, Louis de Broglie proposed something almost embarrassingly reasonable: maybe a particle is just a particle, and it rides a wave. The particle goes through one slit. Its wave goes through both. The wave ripples, interferes, and steers the particle into the stripes. No dice, no paradox. A mechanism. The room — Bohr, Pauli, Heisenberg at the peak of their powers — took it apart. Pauli hit him with a technical objection; de Broglie, underprepared, folded.
For the next twenty-five years the field believed this kind of picture had been proven impossible, on the strength of a celebrated proof by John von Neumann. A young mathematician named Grete Hermann pointed out in 1935 that the proof assumed what it was proving. Nobody listened to her either. The argument wasn't lost; it was adjourned without anyone checking the paperwork.
Then in 1952 David Bohm — pushed out of American physics in the McCarthy purges, working from exile in Brazil — rebuilt the whole theory from scratch, in full detail, and it worked. Same predictions as textbook quantum mechanics, everywhere, forever; but underneath, particles with real positions riding a real wave, watched or not. John Bell — of the famous theorem — read Bohm and never got over it: "In 1952 I saw the impossible done." Bell spent years asking why nobody had told him this theory existed.
So why isn't everyone a Bohmian? One honest reason, one embarrassing one. Honest: the wave lives in a huge abstract space and steers every particle based on where all of them are, instantly, across any distance — [[nonlocality]], worn openly. (Bell later proved every quantum theory pays something like this. Pilot wave is just the one that itemizes the bill.) Embarrassing: momentum. Careers were built elsewhere, the argument was declared over, and nobody likes reopening a settled case. The theory didn't lose. It got outvoted.
The argument
- “It makes the same predictions with extra machinery. Unnecessary.”
- And Many-Worlds makes the same predictions with extra universes. Everybody pays. I pay in machinery you can draw.
- “The wave pushes the particle around, but the particle never pushes back. What kind of physics is that?”
- Strange physics. Strange isn't wrong — show me the experiment it fails. (Quietly: Bohmians argue about this one at their own conferences. We just don't do it in front of you.)
- “Bell's theorem killed hidden variables.”
- Bell's theorem killed local hidden variables, and Bell himself was this theory's loudest defender. He proved my theory has to be nonlocal. It is. Openly. Next.
The experiment
Reconstructed average photon trajectories · 2011
In 2011, a Toronto lab gently tracked thousands of photons through a double slit — soft measurements, easy does it — and drew the average paths. The picture that came out looks *exactly* like the pilot-wave drawing from 1927: smooth lanes, flowing through the slits, braiding into stripes. It doesn't prove the theory. But nobody expected the picture to look that good.
Kocsis, Steinberg et al., Science
The books
What Is Real? by Adam Becker — the closest thing you'll get to a vindication tour. Then Quantum Mechanics and Experience by David Z Albert if you want the machinery.
Your neighbors
Spontaneous Collapse — the other mechanism-lover — but theirs can be caught by an experiment.
Many-Worlds — your fellow wave-realist — kept the wave and fired the particle.
Glossary 24 terms
- wavefunction
-
The mathematical object that assigns a complex number to every possible configuration of a system.
Written ψ. It is not a wave in space like a ripple on a pond — for two particles it lives in a six-dimensional configuration space, not in the room. Whether ψ is a real physical thing or a bookkeeping device for what you know is precisely what the interpretations argue about.
- amplitude
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A complex number whose squared magnitude gives a probability.
Amplitudes are what makes quantum mechanics quantum. Because they are complex, they can cancel — two ways of reaching the same outcome can add up to no chance of it happening at all. Classical probabilities can never do this.
See also: Born rule, interference
- Born rule
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The recipe that turns amplitudes into probabilities: probability equals the amplitude's magnitude squared.
Max Born added it in a footnote in 1926 and won a Nobel Prize for the footnote. Every interpretation has to reproduce it, and several struggle to explain why it holds rather than simply assuming it.
See also: amplitude
- superposition
-
A state that is a combination of other states, with amplitudes attached.
Commonly mangled as "being in two places at once." More accurately: the system is in one perfectly definite state, which happens not to be a state of definite position (or spin, or whatever you are about to measure). The indefiniteness is relative to the question you ask.
See also: eigenstate, interference
- eigenstate
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A state with a definite value for some particular observable.
A state is only ever an eigenstate with respect to a specific question. Definite momentum means wildly indefinite position, and vice versa. There is no state that is definite about everything.
See also: superposition
- interference
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Amplitudes for different paths adding or cancelling, producing fringes.
The double slit is the canonical case: close one slit and the bright band at a given spot can appear, open both and it can vanish. Adding a second way for something to happen made it stop happening. No probability theory built on ordinary numbers does this.
See also: amplitude, decoherence
- the measurement problem
-
Unitary evolution never produces a single definite outcome, yet we only ever see one.
The Schrödinger equation is linear and deterministic, so a measuring device interacting with a superposition should end up in a superposition of readings. It doesn't — you see one number. Every interpretation on this quiz is, at bottom, a different answer to this one problem.
See also: unitary, collapse, decoherence
- collapse
-
The postulated jump from a superposition to a single definite outcome on measurement.
In textbook quantum mechanics it is simply an extra rule bolted alongside the Schrödinger equation, with no account of when it applies or what counts as a measurement. Interpretations either explain it, deny it happens, or make it a real physical process with its own dynamics.
See also: the measurement problem, spontaneous collapse
- decoherence
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Interaction with the environment rapidly destroying interference between branches.
Real and experimentally confirmed, and it explains why you never see a superposed cat. But it does not by itself solve the measurement problem, however often it is claimed to: it explains why the branches stop interfering, not why you end up in exactly one of them.
See also: the measurement problem, interference
- unitary
-
Evolution that is reversible and preserves total probability — the Schrödinger equation.
Unitary dynamics never destroys information and never singles out an outcome. An interpretation that insists dynamics is always unitary (Many-Worlds) must therefore explain single outcomes some other way; one that admits non-unitary collapse must say when and why.
See also: the measurement problem, collapse
- ontic
-
About what exists, independently of anyone's knowledge.
An ontic reading of the wavefunction says ψ is a real physical thing, as much a part of the furniture of the world as a field. Pilot Wave and spontaneous collapse are ontic about ψ.
See also: epistemic, the PBR theorem
- epistemic
-
About what someone knows, rather than about the world itself.
An epistemic reading says ψ encodes an observer's information, so "collapse" is just updating your beliefs — no more mysterious than a probability changing when you look at a card. QBism takes this furthest. The PBR theorem is the main obstacle in its path.
See also: ontic, the PBR theorem, QBism
- locality
-
Nothing here is influenced by a choice made far away, faster than light could carry the news.
Give this up and you can keep definite pre-existing properties. Keep it and you must give up something else. This is the central trade in the whole subject.
See also: Bell's theorem, entanglement
- entanglement
-
A joint state of two systems that cannot be written as one state for each.
The pair has a definite state while neither member does. Measuring one instantly fixes what the other will give — but you cannot use it to send a message, because each side alone sees nothing but noise until the results are compared.
See also: Bell's theorem, locality
- Bell's theorem
-
No theory that is both local and assigns pre-existing values can reproduce quantum predictions.
John Bell showed in 1964 that such theories obey an inequality that quantum mechanics violates. Experiments — Aspect, then loophole-free tests in 2015, Nobel Prize in 2022 — come down on quantum mechanics' side. It is the closest thing here to a settled result, and it is what forces every interpretation to give something up.
See also: locality, hidden variables, superdeterminism
- contextuality
-
An outcome can depend on what else you chose to measure alongside it.
The Kochen–Specker theorem (1967) shows you cannot consistently assign definite values to all observables at once, independently of context. Bell rules out locality plus definite values; this rules out context-independence as well, even setting distance aside.
See also: Bell's theorem, hidden variables
- the PBR theorem
-
Under modest assumptions, the wavefunction cannot be merely information about a deeper real state.
Pusey, Barrett and Rudolph (2012) showed that if systems have real underlying states and independently prepared systems are independent, then ψ must be ontic. Escaping it means denying one of those assumptions — which is exactly what QBism does, by denying there is an underlying state to be ignorant of.
- no-go theorem
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A proof that a whole class of theories cannot reproduce quantum mechanics.
Bell, Kochen–Specker, PBR and Frauchiger–Renner are the big ones. Together they have closed every exit marked "common sense." This is why no interpretation is sane: sanity was ruled out, and all that remains is choosing which strangeness you prefer.
See also: Bell's theorem, contextuality, the PBR theorem, Wigner's friend
- Wigner's friend
-
A thought experiment where an observer is themselves in superposition, as seen by someone outside.
The friend, inside a sealed lab, sees a definite outcome. Wigner, outside, describes the whole lab — friend included — as superposed. Frauchiger and Renner sharpened this in 2018 into an outright contradiction: you cannot keep universal unitarity, single outcomes and observer agreement all at once.
See also: the measurement problem, no-go theorem
- pilot wave
-
Particles always have definite positions, guided by a real physical wave.
De Broglie proposed it in 1927, Bohm rediscovered it in 1952. It is deterministic, it has no measurement problem, and the double slit becomes an ordinary mechanism. The price is explicit nonlocality — the guiding equation depends instantly on the whole configuration.
See also: hidden variables, locality
- QBism
-
Quantum states are an agent's personal degrees of belief, not descriptions of the world.
Short for Quantum Bayesianism. A wavefunction is your betting position; collapse is you updating on experience. It dissolves the measurement problem at the cost of denying that quantum mechanics describes anything observer-independent at all.
See also: epistemic, the PBR theorem
- spontaneous collapse
-
Collapse is a real physical process that happens at random, all by itself.
Ghirardi, Rimini and Weber (1986) added a tiny random collapse term to the dynamics. One particle collapses about once every hundred million years; a cat, containing about 10²⁷ of them, collapses immediately. Uniquely among these, it is a different theory from quantum mechanics and experiments are closing in on it.
- superdeterminism
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Denying that experimenters' choices are independent of the system being measured.
Bell's theorem quietly assumes the settings you choose are uncorrelated with the hidden variables. Drop that assumption and locality survives. The cost is that the correlation must have been arranged at the beginning of the universe, and that no experiment can ever be a fair test of anything.
See also: Bell's theorem, hidden variables