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arXiv:2611.02547

Performance analysis of cat and GKP breeding protocols with squeezed single-photon input

Yoonha Kim, Jaehak Lee

quant-phSubmitted Nov 2, 2026• Announced Nov 3, 2026
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Abstract

Homodyne breeding is a promising optical route for generating large cat states and Gottesman--Kitaev--Preskill (GKP) grid states, using readily available squeezed-cat states as inputs. We analyze the performance of protocols, using squeezed single-photon seeds, $\hat{S}(r)\ket{1}$, as squeezed-cat resources and propagating them through the same cat-to-GKP breeding pipeline. For a symmetric tree with $N=2^{m_1}$ seeds, the heralded resource state reduces to a state with a polynomial-Gaussian wavefunction controlled by a single effective width, achieving near-unit fidelity with the desired cat resource state. Our analysis yields closed-form even-cat fidelities and an inverse-design rule for the seed squeezing. We apply these resources to GKP breeding, and find a large overlap with a practical GKP state. We also investigate the effects of practical imperfections, including finite homodyne acceptance windows and photon loss. This study shows that squeezed single-photon inputs provide a viable resource assignment for homodyne cat and GKP breeding, replacing the demanding requirement for high-resolution photon-number-resolving heralding with an on-demand single-photon source.

AI Summary

The paper asks how squeezed single photons, $\hat S(r)|1\rangle$, perform as substitutes for squeezed-cat inputs in established optical cat-to-GKP homodyne-breeding protocols, avoiding high-photon-number-resolving heralding. For a symmetric balanced tree with $N=2^{m_1}$ seeds and zero homodyne outcomes, the conditional cat-resource wavefunction is derived as $\psi_N(x)\propto x^N e^{-x^2/(2\sigma_{\rm eff})}$, with $\sigma_{\rm eff}=e^{2r}$. Gaussian-moment calculations give closed-form even-cat fidelities and a one-parameter optimization of seed squeezing. At fidelity $\geq0.99$, the largest target amplitudes are approximately $1.65,2.38,3.31,4.65$ for $N=2,4,8,16$. One-step GKP breeding consumes two such resources. All tested ideal outputs have optimized overlap above $0.99$ with a finite-energy qunaught reference. Their symmetric stabilizer-based effective squeezing ranges from $3.30$ to $7.53\,\mathrm{dB}$ for $4$–$32$ seeds; increasing resource size mainly improves one quadrature. Additional GKP-breeding layers extend the comb and redistribute quadrature squeezing while doubling seed cost per layer. An analytic outcome-polynomial treatment evaluates finite-window probabilities and averaged cat fidelities without sampling. At acceptance half-width $w\simeq1$, fidelities remain above $0.9$, but acceptance falls from $0.42$ at $N=2$ to $1.18\times10^{-6}$ at $N=16$. Loss simulations show increasing fragility with resource size; below approximately $95\%$ transmissivity, $N=8$ outperforms $N=16$ in symmetric GKP squeezing. Limitations include power-of-two trees, squeezing below the cited $9.75\,\mathrm{dB}$ fault-tolerance benchmark, and no complete generation-rate model. Finite-window GKP-fusion performance is not established; quoted GKP squeezing uses ideal conditioning.

Little sign of AI-generated textIncrementalStrong assumptions

Central claim may not hold: The paper does not establish GKP output quality and total success probability for finite homodyne acceptance windows throughout the complete cat-to-GKP pipeline. The abstract's practical viability conclusion exceeds the demonstrated end-to-end performance because finite-window preparation, GKP quality, and loss are not evaluated together, and a complete generation-rate model remains open.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

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•Mar 5, 2019•5 citations
Homodyne breeding is a promising optical route for generating large cat states and Gottesman--Kitaev--Preskill (GKP) grid states, using readily available squeezed-cat states as inputs. We analyze the performance of protocols, using squeezed single-photon seeds, S^(r)∣1⟩\hat{S}(r)\ket{1}S^(r)∣1⟩, as squeezed-cat resources and propagating them through the same cat-to-GKP breeding pipeline. For a symmetric tree with N=2m1N=2^{m_1}N=2m1​ seeds, the heralded resource state reduces to a state with a polynomial-Gaussian wavefunction controlled by a single effective width, achieving near-unit fidelity with the desired cat resource state. Our analysis yields closed-form even-cat fidelities and an inverse-design rule for the seed squeezing. We apply these resources to GKP breeding, and find a large overlap with a practical GKP state. We also investigate the effects of practical imperfections, including finite homodyne acceptance windows and photon loss. This study shows that squeezed single-photon inputs provide a viable resource assignment for homodyne cat and GKP breeding, replacing the demanding requirement for high-resolution photon-number-resolving heralding with an on-demand single-photon source.
The paper asks how squeezed single photons, S^(r)∣1⟩\hat S(r)|1\rangleS^(r)∣1⟩, perform as substitutes for squeezed-cat inputs in established optical cat-to-GKP homodyne-breeding protocols, avoiding high-photon-number-resolving heralding.
For a symmetric balanced tree with N=2m1N=2^{m_1}N=2m1​ seeds and zero homodyne outcomes, the conditional cat-resource wavefunction is derived as ψN(x)∝xNe−x2/(2σeff)\psi_N(x)\propto x^N e^{-x^2/(2\sigma_{\rm eff})}ψN​(x)∝xNe−x2/(2σeff​), with σeff=e2r\sigma_{\rm eff}=e^{2r}σeff​=e2r. Gaussian-moment calculations give closed-form even-cat fidelities and a one-parameter optimization of seed squeezing. At fidelity ≥0.99\geq0.99≥0.99, the largest target amplitudes are approximately 1.65,2.38,3.31,4.651.65,2.38,3.31,4.651.65,2.38,3.31,4.65 for N=2,4,8,16N=2,4,8,16N=2,4,8,16.
One-step GKP breeding consumes two such resources. All tested ideal outputs have optimized overlap above 0.990.990.99 with a finite-energy qunaught reference. Their symmetric stabilizer-based effective squeezing ranges from 3.303.303.30 to 7.53 dB7.53\,\mathrm{dB}7.53dB for 444–323232 seeds; increasing resource size mainly improves one quadrature. Additional GKP-breeding layers extend the comb and redistribute quadrature squeezing while doubling seed cost per layer.
An analytic outcome-polynomial treatment evaluates finite-window probabilities and averaged cat fidelities without sampling. At acceptance half-width w≃1w\simeq1w≃1, fidelities remain above 0.90.90.9, but acceptance falls from 0.420.420.42 at N=2N=2N=2 to 1.18×10−61.18\times10^{-6}1.18×10−6 at N=16N=16N=16. Loss simulations show increasing fragility with resource size; below approximately 95%95\%95% transmissivity, N=8N=8N=8 outperforms N=16N=16N=16 in symmetric GKP squeezing. Limitations include power-of-two trees, squeezing below the cited 9.75 dB9.75\,\mathrm{dB}9.75dB fault-tolerance benchmark, and no complete generation-rate model. Finite-window GKP-fusion performance is not established; quoted GKP squeezing uses ideal conditioning.
The development of a continuous-variable photonic quantum computer depends on the reliable preparation of high-quality Gottesman-Kitaev-Preskill states. The most promising GKP preparation scheme is the cat breeding protocol, which can generate GKP states deterministically given a source of squeezed cat states, using beam splitters, homodyne detectors and a feedforward displacement. However, analyzing the performance of the protocol under loss is cumbersome due to the exponential scaling of the system. By representing the Wigner function of the input states as a linear combination of Gaussians, we are able to quickly and accurately simulate several rounds of breeding with mixed input states. Using this novel method, we find that optical loss decreases the overall success probability of the protocol, and prohibits the preparation of a fault-tolerant GKP state when the loss exceeds 4\%. Our methodology is available as open-source code.
Gottesman-Kitaev-Preskill (GKP) qubits, known for their exceptional error-correction capabilities, are highly coveted in quantum computing. However, generating optical GKP qubits has been a significant challenge. Measurement-based methods, where a portion of entangled squeezed vacuum modes are measured with photon number resolving detectors heralding a desired state in the undetected modes, have emerged as leading candidates for optical GKP qubit generation due their minimal resource requirements. While the current measurement-based methods can produce high-quality GKP qubits, they suffer from low success probabilities limiting experimental realization. The heart of the problem lies in the duality of photon number resolving measurements, being both the source of nonlinearity needed to generate quality GKP qubits and the component driving down their probability of successful production. Our method, breeding approximate squeezed coherent state superpositions created by generalized photon subtraction, overcomes this problem by supplementing two photon number resolving measurements with a single high success probability homodyne measurement. This scheme achieves success probabilities $\ensuremath{\ge}{10}^{\ensuremath{-}5}$, two orders of magnitude higher than strictly photon number resolving measurement based methods, while still producing states with high fidelity, possessing error-correction capabilities equivalent to up to a 10 dB squeezed GKP qubit. This breakthrough significantly advances the practical use of the optical GKP qubit encoding.
We present an architecture for the generation of GKP states in which quadrature squeezing operations are used to control the average photon number statistics of probabilistic photon number measurements on Gaussian resource states. Specifically, we present an architecture employing a teleportation-based squeezing protocol and polynomial-gate applications integrated into a time-multiplexed multi-mode cluster state to generate cat states with high amplitudes, which are consequently used to generate GKP states with high quadrature effective squeezing. Compared to our previous work, in addition to using squeezing as a resource, the present architecture reduces damping and noise by minimizing the number of homodyne measurements required in GKP state generation. We demonstrate the effectiveness of these improvements - including dynamic input-state resetting and an improved breeding algorithm - by achieving a fault-tolerance threshold of 11.5 dB cluster squeezing using the RHG surface code for error correction, without requiring active switching or photon-number resource states.
Large-amplitude squeezed cat states and high-quality Gottesman-Kitaev-Preskill (GKP) states are essential for effective quantum error correction, yet their optical preparation has been hindered by challenges such as low success probabilities, small amplitudes, and insufficient squeezing. Addressing these limitations, our research introduces scalable optical schemes for the deterministic preparation of large-amplitude squeezed cat states from photon-number states. Fock states have the benefit of producing consistent cat states across all measurement outcomes and intrinsically provides a degree of squeezing. Notably, these squeezed cat states facilitate the deterministic generation of high-quality approximate GKP states via "breeding," showing that GKP error correction in optics is technically feasible in near-term experiments. Our schemes allow fault-tolerant quantum computation through the use of GKP error correction.
GKP states enable fault-tolerant CV quantum computation, but their generation remains experimentally challenging due to their highly non-Gaussian and infinite-energy ideal structure. In this work, we present a realistic and scalable protocol for generating finite-energy resource states, specifically the qunaught state, using Schrodinger cat states generated in a strongly coupled quantum dot-cavity system. Our scheme combines deterministic squeezed cat-state generation, cat-breeding protocols, and homodyne measurements. Using numerical simulations, we analyze the role of various parameters of the quantum dot-cavity system in the generation of practical qunaught states. Furthermore, we quantify the trade-off between the fidelity and generation probability of these states and exploit the fact that accepting a structured set of homodyne outcomes can significantly enhance the overall success rate. The proposed approach is compatible with integrated photonics and telecom wavelengths, offering a promising route toward scalable CV quantum information processing.
Continuous-variable quantum-computing (CVQC) is the most scalable implementation of QC to date but requires non-Gaussian resources to allow exponential speedup and quantum correction, using error encoding such as Gottesman-Kitaev-Preskill (GKP) states. However, GKP state generation is still an experimental challenge. We show theoretically that photon catalysis, the interference of coherent states with single-photon states followed by photon-number-resolved detection, is a powerful enabler for non-Gaussian quantum state engineering such as exactly displaced single-photon states and MMM-symmetric superpositions of squeezed vacuum (SSV), including squeezed cat states (M=2M=2M=2). By including photon-counting based state breeding, we demonstrate the potential to enlarge SSV states and produce GKP states.