Traversing Gaussian and non-Gaussian regimes in photonic quantum simulators: a review

Abstract Quantum photonic simulators are pivotal for designing and analyzing quantum photonic circuits that utilize both continuous-variable (CV) and discrete-variable (DV) encodings. This review critically examines the transition from Gaussian to non-Gaussian photonic models and the computational overhead that emerges from simulating systems with more than 20 modes or photon numbers exceeding 10 per mode. Gaussian states; such as coherent and squeezed states, are modeled efficiently using first-moment vectors and covariance matrices of dimension $2n \times 2n$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mn>2</mml:mn> <mml:mi>n</mml:mi> <mml:mo>×</mml:mo> <mml:mn>2</mml:mn> <mml:mi>n</mml:mi> </mml:math> , where n is the number of modes. Non-Gaussian elements like the cubic phase gate $U = \exp (i \gamma \hat{x}^{3})$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>U</mml:mi> <mml:mo>=</mml:mo> <mml:mo>exp</mml:mo> <mml:mo>(</mml:mo> <mml:mi>i</mml:mi> <mml:mi>γ</mml:mi> <mml:msup> <mml:mover> <mml:mi>x</mml:mi> <mml:mo>ˆ</mml:mo> </mml:mover> <mml:mn>3</mml:mn> </mml:msup> <mml:mo>)</mml:mo> </mml:math> and photon-subtracted states demand full Fock space representations and scale exponentially with photon number $d^{2}$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>d</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:math> , where d is the Hilbert space dimension. We analyze simulators including , , and , benchmarking their support for tensor networks (bond dimension D &gt;100), GPU acceleration, thus NVIDIA A100 with 1555 GB/s bandwidth, and SoC implementations such as Edge TPU with 8 TFLOPS. Special focus is given to noise models such as photon loss with transmissivity η , thermal noise modeled with $\bar{n} = 1.5$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>n</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mo>=</mml:mo> <mml:mn>1.5</mml:mn> </mml:math> , and dark count Poisson distributions ( $\lambda = 0.1$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>λ</mml:mi> <mml:mo>=</mml:mo> <mml:mn>0.1</mml:mn> </mml:math> ). The review underscores scalable techniques and hybrid quantum-classical workflows vital for near-term photonic quantum computing.

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Journal
EPJ Quantum Technology
Published
2026-08-14
DOI
https://doi.org/10.1140/epjqt/s40507-026-00496-w
Primary Topic
Quantum Computing Algorithms and Architecture
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article
Field-Weighted Citation Impact
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article

Traversing Gaussian and non-Gaussian regimes in photonic quantum simulators: a review

Leonardo Goliatt, Camila Martins Saporetti, Rodrigo Alves Dias, Dennis Delali Kwesi Wayo et al.
EPJ Quantum Technology
Quantum Computing Algorithms and Architecture
article

Traversing Gaussian and non-Gaussian regimes in photonic quantum simulators: a review

Leonardo Goliatt, Camila Martins Saporetti, Rodrigo Alves Dias, Dennis Delali Kwesi Wayo, Masoud Darvish Ganji
article en

Abstract

Abstract Quantum photonic simulators are pivotal for designing and analyzing quantum photonic circuits that utilize both continuous-variable (CV) and discrete-variable (DV) encodings. This review critically examines the transition from Gaussian to non-Gaussian photonic models and the computational overhead that emerges from simulating systems with more than 20 modes or photon numbers exceeding 10 per mode. Gaussian states; such as coherent and squeezed states, are modeled efficiently using first-moment vectors and covariance matrices of dimension $2n \times 2n$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mn>2</mml:mn> <mml:mi>n</mml:mi> <mml:mo>×</mml:mo> <mml:mn>2</mml:mn> <mml:mi>n</mml:mi> </mml:math> , where n is the number of modes. Non-Gaussian elements like the cubic phase gate $U = \exp (i \gamma \hat{x}^{3})$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>U</mml:mi> <mml:mo>=</mml:mo> <mml:mo>exp</mml:mo> <mml:mo>(</mml:mo> <mml:mi>i</mml:mi> <mml:mi>γ</mml:mi> <mml:msup> <mml:mover> <mml:mi>x</mml:mi> <mml:mo>ˆ</mml:mo> </mml:mover> <mml:mn>3</mml:mn> </mml:msup> <mml:mo>)</mml:mo> </mml:math> and photon-subtracted states demand full Fock space representations and scale exponentially with photon number $d^{2}$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>d</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:math> , where d is the Hilbert space dimension. We analyze simulators including , , and , benchmarking their support for tensor networks (bond dimension D &gt;100), GPU acceleration, thus NVIDIA A100 with 1555 GB/s bandwidth, and SoC implementations such as Edge TPU with 8 TFLOPS. Special focus is given to noise models such as photon loss with transmissivity η , thermal noise modeled with $\bar{n} = 1.5$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mi>n</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mo>=</mml:mo> <mml:mn>1.5</mml:mn> </mml:math> , and dark count Poisson distributions ( $\lambda = 0.1$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>λ</mml:mi> <mml:mo>=</mml:mo> <mml:mn>0.1</mml:mn> </mml:math> ). The review underscores scalable techniques and hybrid quantum-classical workflows vital for near-term photonic quantum computing.

EPJ Quantum TechnologyVol. 13(1)
Universidade Federal de Juiz de Fora (BR), Gachon University (KR), Georgia Institute of Technology (US), Universidade do Estado do Rio de Janeiro (BR)
Conselho Nacional de Desenvolvimento Científico e Tecnológico, Fundação de Amparo à Pesquisa do Estado de Minas Gerais
Openalex Percentile: Top 8%
Quantum Computing Algorithms and Architecture
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