The parity matrix is an intermediate representation to efficiently describe the action of CNOT circuits. They are utilized in CNOT routing algorithms like, e.g., RowCol.
Inputs
CNOT circuit with n qubits
Outputs
n \times n binary matrix P with P_{ij} \in \{0, 1\}
The rows correspond to the input qubits and tell us how they are transformed. E.g., the first row tells us that qubit x_0 is transformed to x_0 \oplus x_3.
Very easy-to-read examples are SWAP circuits that just permute qubits, as the corresponding parity matrix is a permutation matrix.
Korbinian likes simulating quantum systems, whether it be via tensor network methods during his PhD, or with quantum computers at Xanadu. Currently, he works on quantum compilation to make simulation algorithms go brrr.