2021
DOI: 10.1103/physrevresearch.3.043026
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Non-Clifford gate on optical qubits by nonlinear feedforward

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Cited by 17 publications
(19 citation statements)
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“…Û (q, y) = P (tan θ(q)) D √ 2q, √ 2y cos θ(q) − √ 2q tan θ(q) (18) where P (k) = exp [ikx 2 /h] is a shear operation, D is a displacement operation and T is an anti-unitary operation, which transforms x → x and p → −p. The anti-unitary operator is derived from the bra of ancillary state.…”
Section: π(Nqm)mentioning
confidence: 99%
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“…Û (q, y) = P (tan θ(q)) D √ 2q, √ 2y cos θ(q) − √ 2q tan θ(q) (18) where P (k) = exp [ikx 2 /h] is a shear operation, D is a displacement operation and T is an anti-unitary operation, which transforms x → x and p → −p. The anti-unitary operator is derived from the bra of ancillary state.…”
Section: π(Nqm)mentioning
confidence: 99%
“…In continuous-variable MBQC, homodyne measurement is one of the most fundamental and powerful measurement (17). When combined with ancillary states and feedforward, homodyne measurement has an ability to implement fault-tolerant universal quantum computation (18)(19)(20). For example, this combination can implement Clifford operations or Gaussian operations (Fig.…”
mentioning
confidence: 99%
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“…On the other hand, non-Clifford operations required non-Gaussian operations [20]. Recently there has been a proposal where GKP non-Clifford operation is efficiently implemented using nonlinear feedforward system and ancillary state [38]. We can use the entanglement structure of the two-sided tree graph to couple the input with the ancillary state here and implement the adaptive homodyne measurement which results in the non-Clifford gate for GKP qubits after the feedforward operations.…”
Section: Universalitymentioning
confidence: 99%