Quantum eraser
The path was recorded, then the record was read a different way — after the particle had already landed. Do the fringes come back?
NO DETECTIONS YET
0 / 3000 detections
FRINGE VISIBILITY
- ALL
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Detection screen: no detections yet. Fire particles to build a record, then choose what to ask the path marker.
Explained by
Copenhagen
The orthodox viewBetween the source and the click there is no path to revise, so nothing about the later choice reaches backwards. The marker and the particle are one phenomenon; what you may say about it depends on which question the whole arrangement was set up to answer, and that is settled only when the marker is read.
Wheeler's delayed-choice experiment was designed to make this vivid, and his own conclusion was the opposite of the popular one: no elementary phenomenon is a phenomenon until it is registered, so there is no earlier fact about the route for a later decision to alter. Critics grant that this is consistent and press the usual complaint — the account explains the correlations by declining to describe what produced them.
Many Worlds
Everything happensNothing collapses and nothing is undone. The marker becomes entangled with the route, which is what stops the two paths from interfering on the screen. Reading the marker a different way sorts the branches differently — and in each of those branches a fringe pattern was always there, hidden inside the sum.
Marking the path entangles the particle with a second system, and interference between two paths is lost exactly when some other system could tell them apart. Erasing measures that system in a basis that both routes answer equally, so the branches it defines are superpositions of the routes rather than one route each. The apparent puzzle — fringes appearing after the fact — is the ordinary observation that a sum of two opposite fringe patterns is flat.
Pilot Wave
Particles, guidedEvery particle had one definite route the whole time, and the later question cannot change which. What the marker does is entangle the wave with a second system, so the part of the wave that went through the other slit can no longer steer the particle. Erasing does not restore that; it selects a subset of the runs that already happened.
In de Broglie–Bohm the guiding wave always passes both slits. Marking the route makes the two branches of the wave occupy different states of the marker, so they no longer overlap and the guidance equation stops producing fringes. That is a permanent fact about each individual run. What sorting by an erased marker does is pick out the runs whose marker later gave one answer, and within that sub-ensemble the trajectory endpoints happen to be distributed as fringes — a statistical selection, not a retroactive change to any trajectory.
Objective Collapse
Collapse is physicsErasure is possible only while the record is still small. A path marker made of one particle can be re-read; once the record has grown to macroscopic size, the theory says a real physical collapse has settled it, and no later question can reopen it. This is the one interpretation on which erasure has a hard limit rather than a merely practical one.
In standard quantum mechanics erasing gets harder as the record spreads into more degrees of freedom, but nothing forbids it in principle — the obstacle is bookkeeping. GRW and CSL make it a matter of physics: past the collapse scale the superposition is genuinely destroyed, so the subsets can never show fringes again however the marker is interrogated. That is a difference of prediction rather than of story, which is why this family is the one experiments can constrain.
QBism
Probability is personalNothing was erased out in the world, because the wave function was never out there. Learning what the marker says changes what you should expect from the detections you have already recorded — the same way learning one card changes the odds you assign to a hand that was dealt long ago.
For a QBist the delayed choice is not even puzzling: an agent's expectations are updated when the agent learns something, and updating a probability about a past event has never required influencing it. The fringes are a feature of a conditional expectation, not of the screen. Critics accept that this dissolves the mystery cleanly and ask the standing question — what must the world be like, that agents' gambles are constrained in exactly this way?
Relational
Facts are relativeThe marker's record is a fact relative to the marker, and the detection is a fact relative to the screen. Nothing settles what is true relative to you until those records reach you — and sorting is precisely that meeting. There was never a single absolute account of the run for the later choice to rewrite.
Rovelli's account makes the delayed choice unremarkable by denying the assumption that generates the paradox: that there is one observer-independent list of what happened, fixed at the moment of detection. Facts are established in interactions, relative to the systems that interact. Comparing the marker's record with the screen's is a further interaction, and it travels at the speed everything else does. The cost is the absolute account itself.
Consistent Histories
Histories, not measurementsThere are two consistent families of histories here — one that asks which slit, one that asks about the phase — and they cannot be combined into a single description. Choosing what to ask the marker chooses which family you are reasoning in. It does not change the run; a framework is not part of the physical state.
This is one of the places the framework machinery earns its keep. Both families are legitimate and each assigns ordinary probabilities to complete histories; what the formalism forbids is the single-framework question the paradox needs, namely whether the particle went through one slit and produced fringes. Griffiths argues that the delayed-choice puzzles dissolve once that combination is recognised as ill-formed rather than mysterious. The standing objection to the whole approach is that nothing in it says which framework describes the world, only which are permitted.
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