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Quantum Error Correction Continuous Variable States Against Gaussian Noise

In this case, the encoded five wave packets form a five-partite linear cluster entangled state.Error-inThe five encoded wave packets constitute five quantum channels, where the errors possibly occur. Phys. 5, 541–546 (2009).CASArticle32.Lassen, M. J. Rev. http://caribtechsxm.com/quantum-error/quantum-error-correction-with-degenerate-codes-for-correlated-noise.php

The APS Physics logo and Physics logo are trademarks of the American Physical Society. Universal quantum computation with continuousvariable cluster states. A 82, 012319 (2010).CASArticle16.Braunstein, S. ChinaShuhong Hao, Xiaolong Su, Caixing Tian, Changde Xie& Kunchi PengAuthorsSearch for Shuhong Hao in:NPG journals • PubMed • Google ScholarSearch for Xiaolong Su in:NPG journals • PubMed • Google ScholarSearch for

M. & Cory, D. Phys. With a vacuum input state and choosing the optimal gains of gi (i = 1, 2...6) the inseparability criteria will be satisfied for any non-zero squeezing of the ancilla modes. Phys.

Phys. Your cache administrator is webmaster. S.H., X.S. Mod.

Res. Five-wave-packet quantum error correction based on continuous-variable cluster entanglement. Phys. et al.

Phys. According to the standard notation for QEC code1, the presented five-wave-packet code should be expressed by [n, k, d] = [5, 1, 3], where n = 5 denote the number of used wave packets, k = 1 et al. D Phys.

  • The aim of quantum error correction (QEC) is to eliminate or, at least, reduce the hazards resulting from the imperfect channels and to ensure transmission of quantum states with high fidelity1.
  • Here, stands for the transformation of modes k and l on a beam-splitter, the corresponding transformation matrix is given byThe input state is encoded with the four ancilla modes by .
  • A 84, 022339 (2011).CASArticle31.Aoki, T.
  • The presented partial encoding method may simplify the error correction procedure and improve the efficiency of QEC.
  • Rev.
  • Phys.

In the experiment, three amplitude-squeezed states, (m = 1, 3, 4), and a phase-squeezed state, (n = 2) are applied, where r is the squeezing parameter (r = 0 and r = +∞ correspond to no squeezing and perfect Rev. Gaussian error correction of quantum states in a correlated noisy channel. J.

A Phys. http://caribtechsxm.com/quantum-error/quantum-error-correction.php Braunstein and T. Please let us know if you find something weird :-) Suggest a formula Use the search or choose from list: Available Lists Toggle Dropdown All Physics Formulas Basic Physics Formulas (High-School et al.

wrote the paper.Competing interestsThe authors declare no competing financial interests.Corresponding authorCorrespondence to Xiaolong Su.Supplementary informationPDF files1.Supplementary InformationCommentsBy submitting a comment you agree to abide by our Terms and Community Guidelines. presented the first experimental implementation of a Shor-type nine-channel QEC code based on entanglement among nine optical beams, which was the achievable largest entangled state on experiments then31. Rev. click site For the p-displacement error , it is unclear which channel the error comes from since only the phase measurement of detector D2 has output with fluctuation for all five channels (see

Rev. C. Since the errors in channels 1 and 2 do not affect the output state, the obtained fidelity is near unity (0.99).

Rev.

Generated Tue, 25 Oct 2016 01:06:31 GMT by s_wx1085 (squid/3.5.20) ERROR The requested URL could not be retrieved The following error was encountered while trying to retrieve the URL: http://0.0.0.9/ Connection Gate sequence for continuous variable one-way quantum computation. We explore the theoretical bounds of the protocol as well as the expected performance given current knowledge and technology. and C.X.

and K.P. Rev. Differentiating from previous approaches by means of directly transferring existing qubit codes into CV codes, they defined the conditions for yielding a CV QEC code firstly and then searched numerically for navigate to this website Phys.