Experimental simulation of postselected closed timelike curves for decoding scrambled quantum information
Pith reviewed 2026-05-23 06:39 UTC · model grok-4.3
The pith
Postselection on a final measurement lets a quantum circuit decode scrambled information before the information is generated.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
When a quantum circuit is conditioned on a chosen final measurement outcome, the same circuit can be re-interpreted as a paradox-free closed timelike curve that decodes globally scrambled information prior to its initial local encoding; the success probability of this decoding is fixed by out-of-time-ordered correlations.
What carries the argument
Postselected closed timelike curves (PCTCs), which re-interpret an ordinary quantum circuit plus postselection as a consistent time-loop trajectory that recovers scrambled information.
If this is right
- Success probability of the PCTC decoding is governed by out-of-time-ordered correlations.
- The protocol can be executed on present-day cloud quantum processors.
- Conditioned on the postselected outcome, information recovery occurs prior to encoding.
- The circuit supplies a causally consistent simulation of future-to-past scrambled-information retrieval.
Where Pith is reading between the lines
- The same postselection technique might be applied to other scrambling diagnostics beyond out-of-time-ordered correlations.
- If postselection can be replaced by a deterministic operation, the time-loop interpretation would extend to non-postselected circuits.
Load-bearing premise
Postselection on a final measurement outcome can be treated as creating a consistent, paradox-free closed timelike curve that decodes information before the information is encoded.
What would settle it
An experiment in which the observed frequency of the postselected outcome fails to match the independently measured out-of-time-ordered correlation or in which the recovered information is inconsistent with the claimed pre-encoding decoding.
Figures
read the original abstract
Quantum information scrambling (QIS) describes the rapid spread of initially localized information across an entire quantum many-body system through entanglement generation. Once scrambled, the original local information becomes encoded globally, inaccessible from any single subsystem. In this work, we introduce a circuit-based decoding protocol. By utilizing the concept of postselected closed timelike curves (PCTCs), we demonstrate how postselection allows us to interpret an ordinary quantum experiment as an example of a paradox-free trajectory, simulating a consistent time loop and reliable information recovery. Specifically, when conditioned on a final postselected outcome, this experiment can be interpreted as decoding the scrambled information even before the original information is generated. Furthermore, the success probability of the PCTC is governed by out-of-time-ordered correlations, which is a standard measure of QIS. We experimentally implement our protocol on cloud-based Quantinuum and IBM quantum processors. Our approach illuminates a unique quantum task under postselection: the causally consistent simulation of future-to-past scrambled information retrieval.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces a circuit-based protocol that uses postselection on a final measurement outcome to interpret an ordinary quantum circuit as a paradox-free postselected closed timelike curve (PCTC). Conditioned on this outcome, the protocol is claimed to decode scrambled quantum information even before the encoding unitary acts, with the success probability governed by out-of-time-ordered correlations (OTOCs). The protocol is experimentally realized on Quantinuum and IBM quantum processors.
Significance. If the postselection is shown to enforce a self-consistent CTC boundary condition that recovers the input state prior to encoding, the work would provide the first experimental simulation of CTC-assisted decoding in a scrambling context and would establish a direct operational link between OTOCs and postselected success probabilities. This could open a new experimental window on quantum causality and information recovery under postselection.
major comments (2)
- [Protocol description and circuit construction] The central claim that the postselected circuit yields a consistent CTC trajectory whose statistics decode the scrambled state before encoding requires an explicit derivation of the self-consistency condition (analogous to Deutsch or postselected CTC fixed-point equations). No such derivation appears in the protocol section; without it the conditional probabilities may reduce to ordinary postselected teleportation rather than pre-encoding recovery.
- [Success probability and OTOC relation] The statement that the PCTC success probability is governed by OTOCs is presented as a derived result, yet the abstract and protocol text provide no calculation showing that the probability equals a specific OTOC (e.g., the four-point correlator) rather than being tautological with the postselection projector. This relation must be derived explicitly before the claim can be used to interpret the experimental data.
minor comments (3)
- [Figures and experimental implementation] Figure captions and circuit diagrams should explicitly label the postselection measurement and the scrambling unitary so that the causal ordering is unambiguous.
- [Experimental results] The manuscript should include a short comparison table of the observed success probabilities against the theoretically predicted OTOC values for the chosen scrambling unitaries.
- [Introduction] A reference to the original Deutsch CTC model and to postselected teleportation literature would clarify the novelty of the consistency condition used here.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the constructive comments, which help clarify the presentation of the PCTC protocol and its connection to OTOCs. We address each major comment below.
read point-by-point responses
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Referee: [Protocol description and circuit construction] The central claim that the postselected circuit yields a consistent CTC trajectory whose statistics decode the scrambled state before encoding requires an explicit derivation of the self-consistency condition (analogous to Deutsch or postselected CTC fixed-point equations). No such derivation appears in the protocol section; without it the conditional probabilities may reduce to ordinary postselected teleportation rather than pre-encoding recovery.
Authors: We agree that an explicit derivation of the self-consistency condition is required to rigorously establish the PCTC interpretation. The manuscript constructs the circuit to simulate a paradox-free trajectory under postselection but does not derive the fixed-point equation in the protocol section. In the revised version we will add this derivation, showing how the postselected measurement enforces the boundary condition that recovers the input state prior to the encoding unitary, thereby distinguishing the protocol from standard postselected teleportation. revision: yes
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Referee: [Success probability and OTOC relation] The statement that the PCTC success probability is governed by OTOCs is presented as a derived result, yet the abstract and protocol text provide no calculation showing that the probability equals a specific OTOC (e.g., the four-point correlator) rather than being tautological with the postselection projector. This relation must be derived explicitly before the claim can be used to interpret the experimental data.
Authors: We acknowledge that the manuscript states the success probability is governed by OTOCs without supplying the explicit calculation linking it to a four-point correlator. We will add this derivation in the revised manuscript, computing the postselection probability in terms of the relevant OTOC to enable direct interpretation of the Quantinuum and IBM experimental results. revision: yes
Circularity Check
No significant circularity; derivation remains self-contained
full rationale
The paper presents a circuit-based protocol that interprets postselected measurements as simulating paradox-free PCTC trajectories for pre-encoding recovery of scrambled information, with success probability stated to be governed by OTOCs. This link is framed as using a pre-existing standard measure of QIS rather than deriving the probability from a fitted parameter or self-referential definition. No equations or steps in the abstract reduce the central interpretive claim or experimental results to an input by construction; the quantum-processor implementation supplies an independent empirical test. The postselection consistency assumption is an interpretive modeling choice, not a self-definitional equivalence. The derivation chain therefore does not collapse under any of the enumerated circularity patterns.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Postselection on quantum measurement outcomes can be interpreted as realizing a paradox-free closed timelike curve
- standard math Out-of-time-ordered correlations quantify quantum information scrambling
invented entities (1)
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Postselected closed timelike curves (PCTCs)
no independent evidence
Lean theorems connected to this paper
-
IndisputableMonolith/Foundation/ArrowOfTime.leanarrow_from_z unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
when conditioned on a final postselected outcome, this experiment can be interpreted as decoding the scrambled information even before the original information is generated. Furthermore, the success probability of the PCTC is governed by out-of-time-ordered correlations.
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
the postselection step introduces nonlinear effects that enforce the Novikov self-consistency principle
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
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Our protocol includes three main steps: (1) en- coding quantum information using QIS, (2) time-travel part of the encoded information into the past via a PCTC, and (3) decoding the original information. We begin with Alice (A), who prepares an arbitrary pure quantum state |ψð with Hilbert space dimension dA at time T1. As time progresses from T1 to T2, sy...
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If the initial state of E and E’ at T0 is a maximally entangled state, E’ can be interpreted as a mirror of E that travels backward in time [ 55, 56]. Fur- 3 thermore, it is necessary to perform a projective (or se- lective) measurement on the joint system EE’ at T2, and the measurement outcome must remain consistent with itself (the same state) at T0 to ...
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can be di- rectly calculated by the success probability P(ψ) of time travel in our decoding protocol [ 47]: Oavg = ∫ ∫ dW dV O(W, V ) = ∫ dψP(ψ) (10) (see Methods). Here, the double integral represents the Haar average over all unitary operators W and V on the corresponding subsystems, and the single integral aver- ages over all initial states |ψð in our ...
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Note that the calibration data of this processor is presented in the Supplementary Information
The circuit is imple- mented using Quantinuum H1-1 quantum charge-coupled processor, which features 20 trapped-ion ( 171Yb+) qubits with all-to-all connectivity [ 73]. Note that the calibration data of this processor is presented in the Supplementary Information. In the following, we explain the circuit in detail in the laboratory’s rest frame (from T0 to...
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with dA = 2: |Φ+ðEE’ = 1√ 2 (|0ðE ¹ |0ðE’ + |1ðE ¹ |1ðE’) , (11) which is a Bell state [ 74]. After applying the decoding operation U † to the joint system HE, we perform quantum state tomography (i.e., single-qubit Pauli measurements [ 74]) on qubit B before T1. To ensure the information is from the future, we reset qubit B and then prepare a pure quantu...
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The success probability for an arbitrary state |ψð under the scrambler Uq is P(ψ) = 0 .25. According to Eq. ( 8), this leads to an estimated fidelity of unity for any state |ψð, indicating perfect decoding. FIG. 4. Circuit representation of the three-qubit Clif- ford scrambler. This scrambling unitary operator includes six controlled- Z and three Hadamard ...
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2(a)], the unitary operator W in Eq
Because the EPR projection oper- ator is applied to the joint system EE’ at T2 [as shown in Fig. 2(a)], the unitary operator W in Eq. ( 19) should act on system E. Therefore, the OTOC ïW †(t)V †W (t)V ð in Eq. ( 21) can be interpreted as the overlap between the following two states: WE(t)VA|φ0ðA ¹ |EPRðEE’ ¹ |EPRðHH’ =U † HE→BHWEUAH→HEVA × |φ0ðA ¹ |EPRðEE...
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is reversed. As time proceeds backward from T1 to T0, Bob encodes the state |φ0ðB into the joint system HE using the scrambling operation ( U † BH→HE)† = UBH→HE. After system E trav- els forward in time from T0 to T2 through the PCTC, the perturbation WE is applied to system E, and the tempo- ral direction is again reversed at T2. As time proceeds backwar...
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