Table 1 Characteristic of single CZ gate on metasurface

From: Quantum CZ gates on a single gradient metasurface

(a) Encoding rules of polarization qubits

 

Control

Target

Auxiliary

Polarization state

\({| R\left.\right\rangle }_{0}\)

\({| L\left.\right\rangle }_{0}\)

\({| R\left.\right\rangle }_{+1}\)

\({| L\left.\right\rangle }_{+1}\)

\({| R\left.\right\rangle }_{+2}\)

\({| L\left.\right\rangle }_{-1}\)

Encoded qubit state

\({| 0\left.\right\rangle }_{C}\)

\({| 1\left.\right\rangle }_{C}\)

\({| 1\left.\right\rangle }_{T}\)

\({| 0\left.\right\rangle }_{T}\)

None

None

Mode label

\({\hat{C}}_{0}^{R}\)

\({\hat{C}}_{1}^{L}\)

\({\hat{T}}_{1}^{R}\)

\({\hat{T}}_{0}^{L}\)

\({\hat{V}}^{R}\)

\({\hat{V}}^{L}\)

(b) Truth table of 2-qubit input states

Input

Output

Post-selection probability

\({| 0\left.\right\rangle }_{C}{| 0\left.\right\rangle }_{T}\)

\({| 0\left.\right\rangle }_{C}{| 0\left.\right\rangle }_{T}\)

1/9

\({| 0\left.\right\rangle }_{C}{| 1\left.\right\rangle }_{T}\)

\({| 0\left.\right\rangle }_{C}{| 1\left.\right\rangle }_{T}\)

1/9

\({| 1\left.\right\rangle }_{C}{| 0\left.\right\rangle }_{T}\)

\({| 1\left.\right\rangle }_{C}{| 0\left.\right\rangle }_{T}\)

1/9

\({| 1\left.\right\rangle }_{C}{| 1\left.\right\rangle }_{T}\)

\(-{| 1\left.\right\rangle }_{C}{| 1\left.\right\rangle }_{T}\)

1/9