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Quantum coherent transceivers toward Holevo-limited communications

Volkan Gurses, Suraj Samaga, Elianna Kondylis, Ali Hajimiri

Apr 8, 2026arXiv:2604.07087v1
quant-pheess.SPphysics.app-phphysics.optics
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#100 of 3346 · Quantum Physics
Tournament Score
1555±35
10501750
77%
Win Rate
27
Wins
8
Losses
35
Matches
Rating
5.8/ 10
Significance6
Rigor6.5
Novelty5.5
Clarity7

Abstract

The Holevo limit bounds the channel capacity of a communication channel in which information is encoded in quantum states in a Hilbert space at the transmitter and decoded using quantum measurements at the receiver. Saturating the Holevo limit requires quantum-limited transceivers that either generate quantum states of light or employ quantum-limited measurements. Here, we demonstrate an integrated photonic-electronic quantum-limited coherent receiver (QRX) achieving 14.0 dB shot noise clearance (SNC), 520 μμW knee power, 2.57 GHz 3-dB bandwidth, 3.50 GHz shot-noise-limited bandwidth, and 90.2 dB common-mode rejection ratio (CMRR\mathrm{CMRR}). We scale this design to a 32-channel QRX array with median 26.6 dB SNC\mathrm{SNC}, and automatic CMRR\mathrm{CMRR} correction yielding a median 76.8 dB CMRR\mathrm{CMRR} at minimum. Using the integrated QRX and fiber-optic transmitter, we measure 0.15±0.010.15\pm0.01 dB of squeezing below the shot noise limit, limited by off-chip losses. We propose a squeezed light communication scheme that can surpass the Shannon limit, with a path toward the Holevo limit.

AI Impact Assessments

(3 models)

Scientific Impact Assessment

1. Core Contribution

This paper presents an integrated photonic-electronic quantum-limited coherent receiver (QRX) on a silicon photonics platform and proposes a squeezed light communication architecture that could theoretically surpass the one-quadrature Shannon limit toward the Holevo limit. The key hardware demonstrations include: (1) a single-channel QRX with 14.0 dB shot noise clearance (SNC), 520 μW knee power, 2.57 GHz 3-dB bandwidth, and 90.2 dB CMRR; (2) a 32-channel QRX array with median 26.6 dB SNC and automatic CMRR correction; and (3) measurement of 0.15 ± 0.01 dB of squeezing below shot noise using a fiber-optic transmitter paired with the integrated receiver. The paper also develops a comprehensive theoretical framework connecting coherent receiver design parameters to communications capacity with squeezed light.

2. Methodological Rigor

The paper is methodologically thorough. The dual semi-classical and quantum treatments of coherent detection are carefully developed, and their equivalence for coherent states is explicitly shown—an instructive pedagogical contribution. The design guide translating physical parameters (CMRR, SNC, knee power, bandwidth) into quantum-limited performance metrics is well-structured and practically useful.

The experimental characterization is detailed. The shot noise linearity fit (slope 1.007 ± 0.015) convincingly establishes quantum-limited operation. The CMRR measurement methodology, including the dynamic range extension technique using different LO powers, is carefully described. The 32-channel array characterization with statistical distributions across channels demonstrates manufacturing feasibility.

However, there are notable gaps. The squeezing measurement of only 0.15 dB is extremely modest—the authors acknowledge this is limited by off-chip losses (13.3 dB system loss), but this significantly undermines the practical claim toward Holevo-limited communications. The theoretical projections in Figure 6 assume η = 0.99, which requires only 2.7 dB on-chip loss and ηopt = 1—conditions far from the demonstrated 13.3 dB system loss. The paper's title promises movement "toward Holevo-limited communications" but the experimental demonstration remains firmly in the classical regime. The proposed communication experiment (Fig. 6a) is described but not actually performed; only the squeezed light detection is demonstrated.

3. Potential Impact

The work has several avenues for impact:

Near-term practical impact: The integrated QRX design with automatic CMRR correction at scale is directly applicable to classical coherent communications, continuous-variable quantum key distribution (CV-QKD), and quantum random number generation. The 32-channel demonstration with uniform performance is a meaningful step toward large-scale quantum photonic systems.

Communications theory: The formal treatment placing squeezed light communications between the Shannon and Holevo limits (Eq. 43) with explicit dependence on parametric gain coefficient μ and detection efficiency η provides a useful design framework. The energy-per-bit analysis identifying crossover regions where squeezing provides net advantage is practically informative.

Platform development: Silicon photonics integration of quantum-limited receivers with co-designed electronics addresses a genuine bottleneck in scaling quantum optical systems. The low knee power (520 μW single-channel, 12.6 μW median for array) enables scaling to many channels from a shared LO.

However, the gap between demonstrated squeezing (0.15 dB) and what's needed for meaningful capacity enhancement (>3 dB) is substantial. The paper relies heavily on projections using parameters from other groups' work rather than demonstrating the full system.

4. Timeliness & Relevance

The work addresses a timely intersection of quantum optics and integrated photonics. As classical coherent communication links approach Shannon limits and datacom/telecom demand increases, alternative approaches gaining even marginal capacity improvements become economically relevant. The emergence of high-efficiency nonlinear waveguides (referenced μ ≈ 224 W^{-1/2} from PPLN microring resonators) makes the proposed squeezed light communications more feasible than even a few years ago. The paper also connects to the growing interest in photonic quantum computing and CV-QKD, where integrated balanced homodyne detectors are essential components.

5. Strengths & Limitations

Strengths:

  • Comprehensive theoretical framework unifying semi-classical and quantum treatments with clear design guidelines
  • Strong single-channel performance metrics (14.0 dB SNC, 90.2 dB CMRR, 2.57 GHz bandwidth)
  • Demonstration of scalability to 32 channels with automatic CMRR correction—crucial for practical deployment
  • Low knee power enabling massive parallelization
  • Clear identification of μ and η as the two governing parameters for squeezed light communications advantage
  • Limitations:

  • The 0.15 dB squeezing measurement is marginal and limited by off-chip components, not by the receiver itself—making this more of a receiver demonstration than a transceiver demonstration
  • The communication experiment is proposed but not executed; no actual data transmission is demonstrated
  • Theoretical projections assume η = 0.99, whereas demonstrated system efficiency is only ~4.6% (η = 0.046)
  • The claim of "toward Holevo-limited communications" requires collective measurements that are not addressed experimentally; squeezed light with coherent detection cannot reach the Holevo limit
  • Reference [24] is listed as "manuscript in preparation," which weakens the theoretical framework it supports
  • Comparison with competing approaches (e.g., Tasker et al.'s 9 GHz detector, Bruynsteen et al.'s 20 GHz detector) could be more explicit regarding where this work advances the state of the art versus where it falls short
  • Overall Assessment:

    This paper makes a solid engineering contribution in integrated quantum-limited coherent receivers with good scalability, but the scientific narrative overpromises relative to what is experimentally demonstrated. The theoretical framework is valuable, but the experimental gap between 0.15 dB measured squeezing and the regime needed for meaningful capacity gain (multiple dB) is large. The work is best understood as an enabling platform demonstration rather than a demonstration of squeezed light communications.

    Rating:5.8/ 10
    Significance 6Rigor 6.5Novelty 5.5Clarity 7

    Generated Apr 9, 2026

    Comparison History (35)

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    claude-opus-4-6·Apr 9, 2026
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