Coherent-state c-q code 

Description

Bosonic c-q code whose codewords form a constellation of coherent states. Encodes real numbers into coherent states for transmission over a quantum channel and decoding with a quantum-enhanced receiver.

The codes consists of \(K\) coherent states on \(n\) modes, where the \(j\)th state, or codeword, is uniquely defined through the amplitude vector \(\boldsymbol{\alpha}^j=(\alpha_1^j, \alpha_2^j, \cdots, \alpha_n^j)\). The codebook, \begin{align} C=\left(\begin{array}{c} \boldsymbol{\alpha}^{1}\\ \vdots\\ \boldsymbol{\alpha}^{K} \end{array}\right)=\left(\begin{array}{cccc} \alpha_{1}^{1} & \alpha_{2}^{1} & \dots & \alpha_{n}^{1}\\ \vdots & \vdots & \ddots & \vdots\\ \alpha_{1}^{K} & \alpha_{2}^{K} & \dots & \alpha_{n}^{K} \end{array}\right)~, \tag*{(1)}\end{align} collects each codeword into the matrix \(C\) that characterizes the system of states to discriminate.

From the properties of \(C\), we can assess whether it is possible to optimally discriminate the codebook unambiguously. Optimal unambiguous state discrimination requires each vector to be linearly independent, which corresponds to a full-rank codebook. This is possible only if \(K \leq n\).

Rate

Random Gaussian-distributed coherent-state c-q codes achieve the capacity of the lossy bosonic channel [1].

Decoding

Optimal receiver performance in ambiguous state discrimination is determined using the Yuen-Kennedy-Lax (YKL) conditions [2]. See review [3] for details on receivers used for coherent-state c-q codes.Joint-detection receiver that can attain channel capacity [4].Various near-optimal receiver designs that can handle arbitrary constellations of coherent states with possible degeneracies [5].The square-root measurement is optimal for geometrically uniform [6–8], direct sums of geometrically uniform [9], and compound geometrically uniform [10] constellations.

Realizations

Continuous-variable quantum key distribution (CV-QKD) [11–13].

Notes

See book [14].

Parent

Children

Cousins

  • Coherent-state constellation code — Coherent-state c-q codes encode classical alphabets into constellations of coherent states, while coherent-state constellation codes encode quantum information into superpositions of coherent states.
  • Modulation scheme — Coherent-state c-q codes are modulation schemes to transmission of classical information over quantum analog channels.
  • Two-component cat code — Two-component cat codes can be thought of as coherent-state c-q codes because they protect against only one type of noise and thus only reliably store classical information.

References

[1]
V. Giovannetti, S. Guha, S. Lloyd, L. Maccone, J. H. Shapiro, and H. P. Yuen, “Classical Capacity of the Lossy Bosonic Channel: The Exact Solution”, Physical Review Letters 92, (2004) arXiv:quant-ph/0308012 DOI
[2]
H. Yuen, R. Kennedy, and M. Lax, “Optimum testing of multiple hypotheses in quantum detection theory”, IEEE Transactions on Information Theory 21, 125 (1975) DOI
[3]
I. A. Burenkov, M. V. Jabir, and S. V. Polyakov, “Practical quantum-enhanced receivers for classical communication”, AVS Quantum Science 3, (2021) DOI
[4]
S. Guha, “Structured Optical Receivers to Attain Superadditive Capacity and the Holevo Limit”, Physical Review Letters 106, (2011) arXiv:1101.1550 DOI
[5]
J. S. Sidhu, M. S. Bullock, S. Guha, and C. Lupo, “Linear optics and photodetection achieve near-optimal unambiguous coherent state discrimination”, Quantum 7, 1025 (2023) arXiv:2109.00008 DOI
[6]
Y. C. Eldar and G. D. Forney Jr, “On Quantum Detection and the Square-Root Measurement”, (2000) arXiv:quant-ph/0005132
[7]
Y. C. Eldar, A. Megretski, and G. C. Verghese, “Optimal Detection of Symmetric Mixed Quantum States”, (2002) arXiv:quant-ph/0211111
[8]
M. Rosati, “Performance of Coherent Frequency-Shift Keying for Classical Communication on Quantum Channels”, 2021 IEEE International Symposium on Information Theory (ISIT) (2021) arXiv:2203.09822 DOI
[9]
N. Dalla Pozza and G. Pierobon, “Optimality of square-root measurements in quantum state discrimination”, Physical Review A 91, (2015) arXiv:1504.04908 DOI
[10]
H. Krovi, S. Guha, Z. Dutton, and M. P. da Silva, “Optimal measurements for symmetric quantum states with applications to optical communication”, Physical Review A 92, (2015) arXiv:1507.04737 DOI
[11]
P. van Loock and S. L. Braunstein, “Unconditional teleportation of continuous-variable entanglement”, Physical Review A 61, (1999) arXiv:quant-ph/9907073 DOI
[12]
F. Grosshans and P. Grangier, “Continuous Variable Quantum Cryptography Using Coherent States”, Physical Review Letters 88, (2002) arXiv:quant-ph/0109084 DOI
[13]
F. Grosshans, G. Van Assche, J. Wenger, R. Brouri, N. J. Cerf, and P. Grangier, “Quantum key distribution using gaussian-modulated coherent states”, Nature 421, 238 (2003) arXiv:quant-ph/0312016 DOI
[14]
J. Gazeau, Coherent States in Quantum Physics (Wiley, 2009) DOI
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Zoo Code ID: coherent_state_c-q

Cite as:
“Coherent-state c-q code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2023. https://errorcorrectionzoo.org/c/coherent_state_c-q
BibTeX:
@incollection{eczoo_coherent_state_c-q, title={Coherent-state c-q code}, booktitle={The Error Correction Zoo}, year={2023}, editor={Albert, Victor V. and Faist, Philippe}, url={https://errorcorrectionzoo.org/c/coherent_state_c-q} }
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“Coherent-state c-q code”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2023. https://errorcorrectionzoo.org/c/coherent_state_c-q

Github: https://github.com/errorcorrectionzoo/eczoo_data/edit/main/codes/classical_into_quantum/oscillators/coherent_state/coherent_state_c-q.yml.