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Violaris' Unitary Message-Transfer Primitive

Updated 28 January 2026
  • Violaris' Unitary Message-Transfer Primitive is a quantum-circuit protocol that conditionally transfers classical messages across branches in a coherent, Wigner’s-friend-style setup.
  • It uses a fixed sequence of CNOT and Pauli-X gates to implement branch encoding, message writing, copying, and uncomputation, ensuring parallelizable operations and controlled circuit depth.
  • Benchmark results across multiple superconducting architectures reveal message pattern-dependent performance, illustrating trade-offs between decoherence, compilers’ routing overhead, and circuit fidelity.

Violaris' Unitary Message-Transfer Primitive (UMP) defines a quantum-circuit protocol for effecting the conditional transfer of a classical message between "branches" in a Wigner's-friend-style circuit under coherent, globally unitary evolution. It provides an operational benchmark for inter-branch communication, with implementations on superconducting quantum hardware spanning up to n=32n=32-qubit messages and multi-architecture comparisons. The UMP serves as both a hardware stress-test and a probe of decoherence, circuit compilation efficiency, and device-dependent error sources in near-term quantum processors (Cogburn, 27 Jan 2026, Altman, 22 Jan 2026).

1. Formal Definition and Operator Structure

The UMP is realized in a specific register ordering: QQ (the branch/measurement qubit) \otimes RR (branch label/reference) \otimes FF (friend’s state) \otimes MM1MnM \equiv M_1 \ldots M_n (n-qubit memory) \otimes PP1PnP\equiv P_1\ldots P_n (paper/message register). The ideal message-transfer unitary QQ0 is a fixed composition of CNOT and Pauli-X gates:

QQ1

with:

  • QQ2
  • QQ3
  • QQ4
  • QQ5
  • QQ6
  • QQ7

In compact operator form:

QQ8

This ordering enforces strict sequential logic on message preparation, branch encoding, writing, copying, uncomputation, and final register swaps (Cogburn, 27 Jan 2026).

2. Gate-Level Decomposition and Two-Qubit Depth Scaling

In superconducting-device implementations (e.g., IBM Qiskit backends), the UMP circuit arranges the logical operations for efficient compilation within hardware connectivity constraints. For message size QQ9:

  • Top three wires: \otimes0, \otimes1, \otimes2 execute sequential CNOTs and single-qubit \otimes3 gates.
  • Next \otimes4 wires (\otimes5): each receives a CNOT from \otimes6 (write), a CNOT to \otimes7 (copy), and a reverse CNOT from \otimes8 (uncompute).
  • Bottom \otimes9 wires (RR0): participate in pairwise (copy/uncompute) CNOTs.

The critical efficiency feature is that the RR1 CNOTs in the copy/uncompute layers commute, supporting full parallelization for those stages. The overall two-qubit gate depth is:

RR2

where RR3 is set by the logical-to-physical mapping overhead of fanout from RR4 to the RR5 qubits. For message patterns with minimal Hamming weight ("sparse"), RR6, yielding constant-depth circuits. For half-weight and dense patterns, RR7, so depth grows linearly in RR8 (Cogburn, 27 Jan 2026).

3. Message Families and Compilation Cost

The benchmarking campaign distinguishes three message patterns RR9:

  • Sparse (“one-hot”): \otimes0. Only one \otimes1 is flipped; \otimes2, compiled depth \otimes3 (constant).
  • Half-weight: Randomly chosen positions, Hamming weight \otimes4; \otimes5, depth \otimes6.
  • Dense (“all-ones”): \otimes7; all \otimes8 active, \otimes9, depth FF0.

On planar superconducting topologies, every non-neighbor CNOT for half/dense families can require SWAP chains, inducing rapidly growing routing overhead. This leads to device- and compiler-seed-dependent variations: transpiler randomness at the coherence-depth frontier becomes a practical limitation for high-weight messages (Cogburn, 27 Jan 2026).

4. Performance Metrics and Diagnostic Observables

Performance evaluation of the UMP is postselected on FF1 (the "message-receiver" branch). The key observables are:

  • Bitwise success: FF2
  • String success ("all-bits"): FF3
  • Memory erasure after uncompute, postselected on FF4: FF5
  • Branch contrast FF6 on active bits: for FF7,

FF8

\otimes0

where \otimes1 is the binary Shannon entropy.

These metrics diagnose both the strict string-level channel performance (\otimes2) and subtler correlations remaining under partial or noisy operation (e.g., \otimes3) (Cogburn, 27 Jan 2026).

5. Multi-Architecture Benchmarking Results

Benchmarks were obtained on IBM Eagle (ibm_rensselaer), Nighthawk (ibm_miami), and Heron r2/r3 (ibm_fez, ibm_boston) processors for \otimes4 up to \otimes5. No error mitigation was applied; all runs used 4096 shots and Qiskit transpiler level 3. Compilation variability was estimated for half/dense messages using randomized seeds.

Table: Maximum \otimes6 with \otimes7 (approximate values):

Backend Dense Half Sparse
ibm_boston 24 32 32
ibm_fez 8 16 32
ibm_miami 16 24 32
ibm_rensselaer 4 8 24

Sparse-family \otimes8 at \otimes9:

  • ibm_rensselaer MM1MnM \equiv M_1 \ldots M_n0
  • ibm_fez MM1MnM \equiv M_1 \ldots M_n1
  • ibm_miami MM1MnM \equiv M_1 \ldots M_n2
  • ibm_boston MM1MnM \equiv M_1 \ldots M_n3

For half/dense messages, MM1MnM \equiv M_1 \ldots M_n4 decreases roughly exponentially with MM1MnM \equiv M_1 \ldots M_n5, illustrating the compounding effects of SWAP/routing-induced decoherence. A noteworthy result is that, for dense messages at MM1MnM \equiv M_1 \ldots M_n6, MM1MnM \equiv M_1 \ldots M_n7 spans from MM1MnM \equiv M_1 \ldots M_n8 (ibm_rensselaer) to MM1MnM \equiv M_1 \ldots M_n9 (ibm_boston).

Bitwise mutual information \otimes0 remains nonzero for dense messages even when \otimes1 at large \otimes2, signifying that some branch–message correlation persists despite an overall loss of string fidelity (Cogburn, 27 Jan 2026).

6. Hardware Noise, Error Sources, and Transpiler Variability

  • Sparse family: Due to constant two-qubit depth (\otimes3), this regime serves as a controlled probe of device-dependent noise; hardware-to-hardware variability in \otimes4 at \otimes5 primarily reflects differences in intrinsic decoherence and CNOT fidelity.
  • Half/dense families: Main limitation is SWAP/routing overhead. As the logical depth increases with message Hamming weight, both device connectivity and randomness in transpiler optimization yield large variations in circuit depth and \otimes6. Close to the coherence frontier, compiler-seed fluctuations can induce order-unity swings in success probability (Cogburn, 27 Jan 2026).

7. Amplitude Sweep, Divergence (“Cousins”) Sweep, and Channel Constraints

The UMP supports protocol-level stress tests probing channel linearity and complexity dependence:

  • Amplitude sweep (no amplification test): By preparing \otimes7 to set \otimes8 and running \otimes9, one obtains PP1PnP\equiv P_1\ldots P_n0. Empirically, the measured marginal weights perfectly track the ideal PP1PnP\equiv P_1\ldots P_n1 relation across all tested backends, indicating no spurious amplification (Cogburn, 27 Jan 2026).
  • Cousins-divergence sweep: A 16-qubit friend state is prepared with Hamming distance PP1PnP\equiv P_1\ldots P_n2 between branches, adding PP1PnP\equiv P_1\ldots P_n3 PP1PnP\equiv P_1\ldots P_n4-gates to PP1PnP\equiv P_1\ldots P_n5. At fixed PP1PnP\equiv P_1\ldots P_n6, sweeping PP1PnP\equiv P_1\ldots P_n7 from PP1PnP\equiv P_1\ldots P_n8 to PP1PnP\equiv P_1\ldots P_n9, the branch contrast QQ00 falls linearly with QQ01, reflecting increased circuit depth and cumulative noise.
  • Channel constraints: In five-qubit (minimal) protocols, additional performance witnesses are defined:
    • Visibility QQ02, extracted from QQ03-basis readout.
    • Coherence witnesses QQ04, QQ05: multi-qubit parities in QQ06 and QQ07 bases, sensitive to off-diagonal coherence.
    • Phase-sensitive magnitude QQ08.

Benchmarks on ibm_fez (QQ09 shots) yield QQ10, QQ11, QQ12, QQ13, compared to ideal QQ14. Visibility is primarily sensitive to population, while QQ15 are directly attenuated by modeled dephasing channels: for QQ16, a dephasing strength QQ17 explains the observed reduction, setting the device constraint on coherence preservation (Altman, 22 Jan 2026).

References

  • M. Violaris, “Quantum observers can communicate across multiverse branches,” (Violaris, 13 Jan 2026) (2026).
  • C. V. Cogburn, "Inter-branch message transfer on superconducting quantum processors: a multi-architecture benchmark," (Cogburn, 27 Jan 2026) (2026).
  • C. V. Cogburn, "Wigner's Friend as a Circuit: Inter-Branch Communication Witness Benchmarks on Superconducting Quantum Hardware," (Altman, 22 Jan 2026) (2026).

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