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arxiv: 2501.16335 · v4 · submitted 2025-01-04 · 🪐 quant-ph

Experimental simulation of postselected closed timelike curves for decoding scrambled quantum information

Pith reviewed 2026-05-23 06:39 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum information scramblingpostselected closed timelike curvesout-of-time-ordered correlationsquantum circuitsquantum processorsinformation decoding
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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.

The paper establishes a circuit protocol in which conditioning on one specific postselected outcome turns an ordinary quantum experiment into a simulation of a closed timelike curve. Under that conditioning the scrambled data can be recovered even though the original local information has not yet been encoded. The probability that the postselected outcome occurs is set by out-of-time-ordered correlations, the usual diagnostic of scrambling. The protocol was run on cloud quantum processors, showing that the time-loop interpretation is experimentally realizable. The result supplies a concrete, causally consistent way to retrieve future-to-past scrambled information when postselection is allowed.

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

These are editorial extensions of the paper, not claims the author makes directly.

  • 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

Figures reproduced from arXiv: 2501.16335 by Adam Miranowicz, Franco Nori, Guang-Yin Chen, Hsiang-Wei Huang, Jhen-Dong Lin, Neill Lambert, Yi-Te Huang, Yueh-Nan Chen.

Figure 1
Figure 1. Figure 1: 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, sys￾tem A interacts with a chronology-respecting many-b… view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2 [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3 [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4 [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
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.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 3 minor

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)
  1. [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.
  2. [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)
  1. [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.
  2. [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.
  3. [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

2 responses · 0 unresolved

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
  1. 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

  2. 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

0 steps flagged

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

0 free parameters · 2 axioms · 1 invented entities

Central claim rests on interpreting postselection as a consistent CTC simulation and on OTOCs as the governing quantity; both are domain-standard but the specific mapping is introduced here.

axioms (2)
  • domain assumption Postselection on quantum measurement outcomes can be interpreted as realizing a paradox-free closed timelike curve
    Invoked to justify the time-loop decoding interpretation
  • standard math Out-of-time-ordered correlations quantify quantum information scrambling
    Standard in the field and used to link success probability to scrambling
invented entities (1)
  • Postselected closed timelike curves (PCTCs) no independent evidence
    purpose: To frame postselected quantum circuits as consistent time-loop simulators for information decoding
    Conceptual construct introduced to enable the before-generation decoding claim

pith-pipeline@v0.9.0 · 5731 in / 1333 out tokens · 26849 ms · 2026-05-23T06:39:05.403194+00:00 · methodology

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Works this paper leans on

89 extracted references · 89 canonical work pages · 2 internal anchors

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    We begin with Alice (A), who prepares an arbitrary pure quantum state |ψð with Hilbert space dimension dA at time T1

    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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    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

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