| Measurement Methods |
|---|
| row1(qc, q_0, q_1, q_meas) |
| row2(qc, q_0, q_1, q_meas) |
| row3(qc, q_0, q_1, q_meas) |
| col1(qc, q_0, q_1, q_meas) |
| col2(qc, q_0, q_1, q_meas) |
| col3(qc, q_0, q_1, q_meas) |
| meas_11_12(qc, q_0, q_1, q_meas) |
| meas_13(qc, q_0, q_1, q_meas) |
| meas_21_22(qc, q_0, q_1, q_meas) |
| meas_23(qc, q_0, q_1, q_meas) |
| meas_31(qc, q_0, q_1, q_meas) |
| meas_32(qc, q_0, q_1, q_meas) |
| meas_33(qc, q_0, q_1, q_meas) |
| meas2_row1(qc, q_0, q_1, q_meas1, q_meas2, q_meas3) |
| meas2_row2(qc, q_0, q_1, q_meas1, q_meas2, q_meas3) |
| meas2_row3(qc, q_0, q_1, q_meas1, q_meas2, q_meas3) |
| meas2_col1(qc, q_0, q_1, q_meas1, q_meas2, q_meas3) |
| meas2_col2(qc, q_0, q_1, q_meas1, q_meas2, q_meas3) |
| meas2_col3(qc, q_0, q_1, q_meas1, q_meas2, q_meas3) |
| Initialization Methods |
|---|
| xxinit(qc, q_0, q_1, q_meas) |
| xyinit(qc, q_0, q_1, q_meas) |
| yxinit(qc, q_0, q_1, q_meas) |
| yyinit(qc, q_0, q_1, q_meas) |
| zxinit(qc, q_0, q_1, q_meas) |
| xzinit(qc, q_0, q_1, q_meas) |
| yzinit(qc, q_0, q_1, q_meas) |
| zyinit(qc, q_0, q_1, q_meas) |
| negzzinit(qc, q_0, q_1, q_meas) |
The first 13 measurement methods take 4 arguments, these are qc, q_0, q_1, and q_meas. qc is the quantum circuit object, and q_0,q_1,q_meas are qubits. Each method corresponds to a quantum circuit which can be easily discerned by the name of the method, e.g the row1 method corresponds to the quantum circuit for the first row in Mermin-Peres Magic Square and so on. meas_11_12 means that the method can be used for the first measurement in the first row and the second measurement in the first row thus reducing redundancy.
The final 6 measurement methods take 6 arguments. As the previous methods the first argument qc is the quantum circuit object and the remaining arguments are qubits to be used. These methods require five qubits as we require three ancilla qubits for the measurements.