Wave function evolution
What does the equation do between measurements?
Unitary — information preserved
forward in time
Paused, pointing forward in time at t equals 0.00, packet width 0.06 of the baseline. The evolution is smooth, deterministic and reversible — running the same interval backwards returns the state exactly to where it began. Measuring is where the interpretations part ways: some add a genuinely irreversible step, others keep the dynamics unitary throughout and call the loss practical rather than fundamental.
Explained by
Copenhagen
The orthodox viewBetween measurements the equation runs the state forward smoothly and reversibly, and Copenhagen uses it without reservation. What it will not say is that the state is a thing evolving out in the world — it is the bookkeeping that yields probabilities when a measurement finally happens.
The orthodox account has two rules: unitary evolution between measurements, and collapse at measurement. Only the first is deterministic and reversible; the second is neither, and the theory never states which applies when. That gap is the measurement problem in one sentence, and every other interpretation on this page is an attempt to remove one of the two rules or to explain how they fit together.
Many Worlds
Everything happensThis is the whole of the physics. The wave function is real, the equation is exact, and nothing else ever happens — so the smooth reversible run you can scrub back and forth here is not an interlude between measurements. It is the entire story.
Everett's proposal is precisely to delete the second rule. Measurement becomes an ordinary interaction in which observer and system become entangled, and what looks like collapse from inside is a record that has branched. Because the dynamics never stop being unitary, information is never destroyed — an assumption that reaches well beyond interpretation, since the same commitment drives the black-hole information debate. What supporters must still supply is why branch weights should be experienced as probabilities.
Pilot Wave
Particles, guidedTwo things evolve here, and both do so deterministically: the wave, which obeys the same equation as everywhere else, and the particle configuration it guides. Run the pair backwards and you arrive exactly where you started — the theory contains no random step at all.
Given the wave function and the initial configuration, de Broglie–Bohm fixes everything that follows. Quantum randomness enters only as ignorance of that initial configuration, distributed according to the Born rule, so what looks like indeterminism is classical-style uncertainty about a starting point. Reversibility holds for wave and particles together. The cost, again, is that the guidance equation depends instantly on the whole configuration however far apart its parts are.
Objective Collapse
Collapse is physicsAlmost, but not quite. On this view the equation is very nearly right: evolution is smooth and reversible except for rare random localization events built into the dynamics themselves. For a single particle they are so rare that the picture here holds for a very long time.
GRW and CSL modify the equation rather than interpreting it, adding a stochastic term whose rate scales with the number of particles involved. Evolution is therefore not exactly unitary and information is not exactly preserved, which is what makes these models testable and what makes reconciling them with relativity difficult. Below the microscopic scale the deviation sits far under anything measurable; for anything macroscopic it dominates completely.
QBism
Probability is personalWhat evolves is an agent's expectation, not the world. Between experiences nothing has been learned, so the rule says how to carry the odds forward coherently — and because no information has entered, that step can be run backwards without loss.
QBism reads unitary evolution as a normative rule for updating a personal state assignment in the absence of new experience, closely analogous to the way a Bayesian carries a probability forward when nothing has been observed. Measurement is the one step that is not reversible, precisely because it is the step where experience arrives and the books are rewritten. What the world is like, such that agents must keep their books this way and no other, is the question QBism leaves open.
Relational
Facts are relativeThe evolving state is always a state relative to something — here, the rest of the laboratory. Between interactions there is nothing to update, so the description runs forward and backward smoothly. It is interaction, not the passage of time, that creates facts.
On Rovelli's account the wave function is not an absolute object but the way one system encodes information about another. Unitary evolution describes that relation while no new interaction occurs; a measurement is an interaction, and it establishes a value relative to the systems involved. Consistency survives because any comparison of two records is itself an interaction. What is given up is the idea of a single observer-independent history into which everything must fit.
Consistent Histories
Histories, not measurementsAmplitudes propagate along histories by the same smooth rule, and nothing is decided while they do. Within a consistent family, probabilities attach to whole histories rather than being created at particular moments — so no instant is privileged as the one where the smooth part stops.
The formalism assigns amplitudes to sequences of events using the unitary dynamics, then checks whether the histories in a family interfere. If they do not, ordinary probabilities apply and measurement appears as physics inside a history rather than as an intervention from outside it. Because probabilities belong to complete histories, the split between smooth evolution and irreversible outcome reflects the family chosen, not the dynamics. The unresolved point is that many incompatible families are equally consistent.
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