Measurement
What turns many possibilities into one result?
Ready, explained by Copenhagen. Nothing has been run yet, so there is no outcome. Press play to run the event.
Explained by
Copenhagen
The orthodox viewBefore the detector fires, the system holds two possible readings with definite weights. The measurement is the moment the description snaps: one reading becomes real; the other was never more than potential. What counts as “the measurement”? Copenhagen deliberately does not say — the arrangement fixes the boundary, and the theory never says at which link in the chain.
The “collapse” here is an update of the description, and the interpretation is split on whether anything physical corresponds to it. Bohr required a classical side to every experiment: apparatus described in laboratory language, quantum system described by amplitudes, with the boundary set by the experimental arrangement rather than chosen at will. The sweep line in this figure is that cut in action — and the standing criticism is that the theory never says where the sweep must happen, only that by the time you read the dial, it has.
Many Worlds
Everything happensNothing snaps. The detector is a quantum system too, and it simply joins the superposition — pointer one way with outcome 0, pointer the other way with outcome 1. Both readings occur, each with a version of you seeing it. The replay you watch here follows one branch, because that is all any observer ever sees.
Decoherence does the work collapse was invented for: once the detector's trillions of degrees of freedom correlate with the system, the two branches stop interfering for all practical purposes. Each branch contains a consistent record — apparatus, environment, memory — so from inside, history looks single. The price is probability: if both outcomes happen, the Born weights need a new justification, and whether the standard arguments succeed is still contested.
Pilot Wave
Particles, guidedThe outcome was never open. The particle had a definite configuration all along, and the measurement merely reveals it. Run the same preparation with the same hidden starting point and the same reading comes out. The apparent randomness is ignorance of initial conditions, not indeterminism in nature.
In de Broglie–Bohm mechanics the guiding wave develops separated packets during measurement, and the particle ends up in exactly one of them — which one being fixed by where it started. The empty packet persists but stops mattering to the particle's future. Quantum randomness becomes classical-style ignorance over initial conditions (quantum equilibrium). The guidance is explicitly nonlocal: entangled partners respond instantly, which is why this theory sits uneasily beside special relativity.
Objective Collapse
Collapse is physicsCollapse is a physical event with a rate. A microscopic system can stay spread out for ages; couple it to a detector of a trillion trillion particles and localization becomes practically instantaneous. No observer is required — the burst you see here fires whether or not anyone looks. When it fires is random, at a rate set by how many particles are caught up in the state; which outcome the localization finds is set by the amplitudes.
GRW-style models add rare, random localization events to the dynamics; CSL makes the process continuous. The collapse rate scales with the size of the entangled system, which turns the quantum–classical boundary into a number. Because the modified dynamics differ slightly from standard quantum mechanics, matter-wave interferometry with ever larger molecules genuinely constrains these models — a rare case where interpretation edges into testable physics. This scene shows a generic, simplified collapse; the specific theories differ in mechanism and rate.
QBism
Probability is personalThe spread-out state was never the system's property — it was your betting book. The detector click is new experience, and the “collapse” is you updating: probabilities in, certainty out. Ask what happened out there between preparation and click, and QBism answers carefully: that question outruns what the formalism is for.
QBism reads the Born rule as a normative constraint on any agent's gambles — a rule of coherence, like logic, not a law of motion. Measurement outcomes are personal experiences, and two agents may lawfully assign different states to the same system until they compare notes — comparing notes being one more measurement.
Relational
Facts are relativeThe detector gains a fact: relative to it, the system now has a value. You, not yet having looked, still correctly describe detector-plus-system in superposition. A fact for one system is not automatically a fact for another — definiteness spreads by interaction, not by decree.
Rovelli's proposal treats every interaction as a measurement for the systems involved, with no super-observer to keep a universal account. How far fact-relativity can be pushed is an active debate — “Wigner's friend” scenarios, where one observer measures another, are exactly the pressure tests, and their interpretation remains unsettled.
Consistent Histories
Histories, not measurementsChoose the family of histories that ends in detector readings, and the formalism hands you ordinary probabilities for each. One history is realized; measurement appears inside it as plain physics. The subtlety is the choice itself: other families were available, and nothing in the theory picks one.
The consistency condition guarantees that a family's history probabilities add up classically, with no interference between them. Within the pointer-reading family, measurement is unmysterious. Across families, descriptions cannot be combined — the “single framework rule” — and critics press on what that rule says about which events actually occur.
Key assumptions
- The wave function is a predictive tool, not an object
- Measurement is a special, unanalysed act
- A classical world of labs and screens is assumed, not derived
What it gets right
- Matches every experiment with the least machinery
- No extra worlds, particles, or equations
- The working physicist's default for a century
What it gets questioned on
- Never says what counts as a measurement
- Puts a movable, unexplained cut through reality
- Not one doctrine — Bohr and Heisenberg never fully agreed
Key assumptions
- The wave function is physically real — and is all there is
- The equation holds always, with no exceptions for observers
- Branching structure emerges through decoherence
What it gets right
- No collapse, no special role for measurement
- Fully deterministic at the level of the whole
- Removes a rule rather than adding equations, supporters argue
What it gets questioned on
- An enormous inventory of worlds no one can see
- The Born rule must be argued for, not assumed
- What exactly counts as one branch?
Key assumptions
- Particles with definite positions at all times
- A real guiding wave obeying the usual equation
- An initial statistical distribution (quantum equilibrium)
What it gets right
- A single definite world — no collapse, no branching
- Observers appear nowhere in the laws
- Recovers the non-relativistic predictions exactly
What it gets questioned on
- Openly nonlocal — awkward with special relativity
- Only position is definite; spin and the rest are contextual
- Extending it to quantum field theory is hard work
Key assumptions
- The wave function is a physical object
- The standard equation is slightly, stochastically wrong
- Collapse rate grows with the number of constituent particles
What it gets right
- Observers play no role at all
- Draws the quantum–classical boundary quantitatively
- Makes predictions that experiments can chase
What it gets questioned on
- The wave function never quite vanishes — the problem of tails
- Standard versions heat matter slowly — later variants patch this
- Each null experiment shrinks its living room
Key assumptions
- Probabilities are personal degrees of belief
- A measurement is an agent's action on the world
- The formalism is a normative rule for betting, not a map
What it gets right
- The measurement problem simply dissolves
- No nonlocal mechanism — updating isn't physics
- Takes the probabilistic core of the theory seriously
What it gets questioned on
- Seems to abandon the third-person picture science expects
- The world between agents is left undescribed
- Critics hear solipsism; QBists insist it is not
Key assumptions
- States describe relations, not intrinsic properties
- Every physical system can serve as an observer
- Facts are complete only relative to an interaction
What it gets right
- No collapse, no extra worlds, no new dynamics
- Dissolves paradoxes by forbidding the view from nowhere
- Kinship with the spirit of relativity
What it gets questioned on
- A world of many partial facts takes getting used to
- Comparing observers' accounts needs delicate care
- Critics ask: relations between what, exactly?
Key assumptions
- Probabilities attach to histories, not measurement outcomes
- Only mutually consistent families of histories may be combined
- The formalism applies to closed systems, observers included
What it gets right
- Measurement loses its special status entirely
- Applies to the whole universe — no outside observer needed
- Stays close to the standard formalism, adding no new dynamics
What it gets questioned on
- No rule selects which framework to use
- Different frameworks license incompatible descriptions
- Critics ask what, if anything, actually happens