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When Jzz 0, the interaction between detuned qubits is not suppressed, and it is preferable to switch off the coupling during single-qubit operations in this case.
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The CNOT operator defined in Eq. (16) specifies qubit 1 to be the control qubit. The locally equivalent alternative controlling the second qubit is SWAP×CNOT×SWAP.
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The CNOT operator defined in Eq. (16) specifies qubit 1 to be the control qubit. The locally equivalent alternative controlling the second qubit is SWAP×CNOT×SWAP.
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26
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75949118889
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We also adopt a slightly different notation than that of Ref. [7], writing c as -2r.
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We also adopt a slightly different notation than that of Ref. [7], writing c as -2r.
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27
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Rμ(θ)ie-i(θ/2)σiμ is a μ rotation on qubit i.
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Rμ(θ)ie-i(θ/2)σiμ is a μ rotation on qubit i.
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75949101011
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Pulse sequences for the XY case were previously derived in unpublished notes by Matthias Steffen.
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Pulse sequences for the XY case were previously derived in unpublished notes by Matthias Steffen.
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