In order to support QMHL for QHBMs whose EnergyFunction does not have a Pauli operator representation, we would need to enable functionality for differentiating the expectation of such energy functions with respect to the parameters of the parameterized quantum circuit.
In order to support QMHL for QHBMs whose EnergyFunction does not have a Pauli operator representation, we would need to enable functionality for differentiating the expectation of such energy functions with respect to the parameters of the parameterized quantum circuit.