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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, &&&1&&&).

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 UmtU_{mt} is a fixed composition of CNOT and Pauli-X gates:

Umt=UswapUuncomputeUwriteUbranchUmeasure,U_{mt} = U_{swap} \cdot U_{uncompute} \cdot U_{write} \cdot U_{branch} \cdot U_{measure},

with:

  • Umeasure=CNOTQFU_{measure} = \mathrm{CNOT}_{Q\rightarrow F}
  • Ubranch=CNOTFRU_{branch} = \mathrm{CNOT}_{F\rightarrow R}
  • Uwrite=i=1nCNOTFMiU_{write} = \prod_{i=1}^n \mathrm{CNOT}_{F\rightarrow M_i}
  • Ucopy=i=1nCNOTMiPiU_{copy} = \prod_{i=1}^n \mathrm{CNOT}_{M_i\rightarrow P_i}
  • Uuncompute=i=1nCNOTPiMiU_{uncompute} = \prod_{i=1}^n \mathrm{CNOT}_{P_i\rightarrow M_i}
  • Uswap=XQXRXFU_{swap} = X_Q \otimes X_R \otimes X_F

In compact operator form:

Umt=(XQXRXF)i=1nCNOTPiMii=1nCNOTMiPiCNOTFRCNOTQFU_{mt} = (X_Q X_R X_F) \cdot \prod_{i=1}^n \mathrm{CNOT}_{P_i \rightarrow M_i} \cdot \prod_{i=1}^n \mathrm{CNOT}_{M_i \rightarrow P_i} \cdot \mathrm{CNOT}_{F \rightarrow R} \cdot \mathrm{CNOT}_{Q \rightarrow F}

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 nn:

  • Top three wires: QQ, RR, FF execute sequential CNOTs and single-qubit XX gates.
  • Next nn wires (M1MnM_1 \ldots M_n): each receives a CNOT from FF (write), a CNOT to PiP_i (copy), and a reverse CNOT from PiP_i (uncompute).
  • Bottom nn wires (P1PnP_1 \ldots P_n): participate in pairwise (copy/uncompute) CNOTs.

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

depth2Q=1 (QF)+1 (FR)+Dwrite+1 (MP copy)+1 (PM uncompute)\text{depth}_{2Q} = 1 \ (\mathrm{Q}\rightarrow \mathrm{F}) + 1 \ (\mathrm{F}\rightarrow \mathrm{R}) + D_{write} + 1\ (\mathrm{M} \to \mathrm{P\ copy}) + 1\ (\mathrm{P} \to \mathrm{M\ uncompute})

where DwriteD_{write} is set by the logical-to-physical mapping overhead of fanout from FF to the MiM_i qubits. For message patterns with minimal Hamming weight ("sparse"), Dwrite=1D_{write}=1, yielding constant-depth circuits. For half-weight and dense patterns, DwriteHamming weightD_{write}\propto Hamming\ weight, so depth grows linearly in nn (Cogburn, 27 Jan 2026).

3. Message Families and Compilation Cost

The benchmarking campaign distinguishes three message patterns μ{0,1}n\mu \in \{0,1\}^n:

  • Sparse (“one-hot”): μ=100\mu = 10\ldots 0. Only one MiM_i is flipped; Dwrite=1D_{write}=1, compiled depth 5\approx 5 (constant).
  • Half-weight: Randomly chosen positions, Hamming weight k=n/2k=\lfloor n/2 \rfloor; DwriteO(n/2)D_{write}\sim O(n/2), depth O(n)O(n).
  • Dense (“all-ones”): μ=111\mu = 11\ldots 1; all MiM_i active, DwritenD_{write}\sim n, depth O(n)O(n).

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 R=0R=0 (the "message-receiver" branch). The key observables are:

  • Bitwise success: pbit=(1/n)i=1nPr[Pi=μiR=0]p_{\text{bit}} = (1/n)\sum_{i=1}^{n} \Pr[P_i = \mu_i | R=0]
  • String success ("all-bits"): pall=Pr[P=μR=0]p_{\text{all}} = \Pr[P=\mu | R=0]
  • Memory erasure after uncompute, postselected on R=1R=1: perase=Pr[M=0nR=1]p_{\text{erase}} = \Pr[M=0^n | R=1]
  • Branch contrast Δ\Delta on active bits: for μi=1\mu_i=1,

Δ=(1/k)i:μi=1[Pr(Pi=1R=0)Pr(Pi=1R=1)]\Delta = (1/k)\sum_{i:\mu_i=1} [\Pr(P_i=1|R=0) - \Pr(P_i=1|R=1)]

  • Bitwise mutual information I(R;Pi)I(R;P_i) (averaged over active bits):

I(R;Pi)=H(Pi)H(PiR)I(R;P_i) = H(P_i) - H(P_i|R)

where HH is the binary Shannon entropy.

These metrics diagnose both the strict string-level channel performance (pallp_{\text{all}}) and subtler correlations remaining under partial or noisy operation (e.g., I(R;Pi)I(R;P_i)) (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 nn up to $32$. 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 nn with pall0.1p_{\text{all}}\geq 0.1 (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 pallp_{\text{all}} at n=32n=32:

  • ibm_rensselaer 0.07\approx 0.07
  • ibm_fez 0.40\approx 0.40
  • ibm_miami 0.52\approx 0.52
  • ibm_boston 0.68\approx 0.68

For half/dense messages, pall(n)p_{\text{all}}(n) decreases roughly exponentially with nn, illustrating the compounding effects of SWAP/routing-induced decoherence. A noteworthy result is that, for dense messages at n=16n=16, pallp_{\text{all}} spans from $0.02$ (ibm_rensselaer) to $0.31$ (ibm_boston).

Bitwise mutual information I(R;Pi)I(R;P_i) remains nonzero for dense messages even when pall0p_{\text{all}}\to 0 at large nn, 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 (5\approx 5), this regime serves as a controlled probe of device-dependent noise; hardware-to-hardware variability in pallp_{\text{all}} at n=32n=32 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 pallp_{\text{all}}. 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 QQ to set Pr(R=0)=p0\Pr(R=0)=p_0 and running UmtU_{mt}, one obtains Pr(R=0)final1p0\Pr(R=0)_{final} \approx 1 - p_0. Empirically, the measured marginal weights perfectly track the ideal 1p01-p_0 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 dd between branches, adding dd XX-gates to UswapU_{swap}. At fixed n=16n=16, sweeping dd from $0$ to $16$, the branch contrast Δ\Delta falls linearly with dd, reflecting increased circuit depth and cumulative noise.
  • Channel constraints: In five-qubit (minimal) protocols, additional performance witnesses are defined:
    • Visibility V=Pr(R=0P=1)Pr(R=1P=1)V = |\Pr(R=0|P=1) - \Pr(R=1|P=1)|, extracted from ZZ-basis readout.
    • Coherence witnesses WXW_X, WYW_Y: multi-qubit parities in XX and YY bases, sensitive to off-diagonal coherence.
    • Phase-sensitive magnitude Cmag=WX2+WY2C_{mag} = \sqrt{W_X^2 + W_Y^2}.

Benchmarks on ibm_fez ($20,000$ shots) yield Vhw=0.877±0.0034V_{hw} = 0.877 \pm 0.0034, WX=0.840±0.0038W_X = 0.840 \pm 0.0038, WY=0.811±0.0041W_Y = -0.811 \pm 0.0041, Cmag=1.167±0.0040C_{mag} = 1.167 \pm 0.0040, compared to ideal Cmag=1.414C_{mag} = 1.414. Visibility is primarily sensitive to population, while WX,WYW_X, W_Y are directly attenuated by modeled dephasing channels: for WX=0.8398W_X = 0.8398, a dephasing strength λest0.08\lambda_{est} \approx 0.08 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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