Table 8 Number of projection measurements required by the proposed scheme to obtain an arbitrary process matrix element for a multi-particle system
From: Efficient non-destructive direct characterization of arbitrary many-body quantum channels
Type of matrix element | Number of projection measurement settings | Explanation |
|---|---|---|
Diagonal Elements \({\chi }_{J,K}^{M,N}(M=N,J=K)\) | 1 | Requires only a single parameter setting. The diagonal element can be directly obtained from one projection probability. |
Off-diagonal Elements (satisfying the mathematical form \({\chi }_{J,K}^{M,N}(M=N,J\,\ne \,K)\) or \({\chi }_{J,K}^{M,N}(M\,\ne \,N,J=K)\)) | 4 | Requires four different parameter settings. The real and imaginary parts of the element are obtained via a linear combination of the four corresponding projection probabilities. |
Off-diagonal Elements (satisfying the mathematical form \({\chi }_{J,K}^{M,N}(M\,\ne \,N,J\,\ne \,K)\)) | 16 | Requires sixteen different circuit parameter settings. The real and imaginary parts are determined through a linear combination of the sixteen corresponding projection probabilities. |