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Quantum Gate Set Tomography
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==Properties== * Figure of merit: Gate set * Multiple copies of the quantum state are required in this method. * <math>E_j</math> should be tomographically complete. * In contrast to QPT, it is not possible in GST to characterize one gate at a time. Instead, GST estimates every gate in the gate set simultaneously. * SPAM gates are included in the gate set for self-consistency. * The limitation of linear-inversion GST (or LGST) is that it does not constrain the estimates to be physical. However, LGST provides a convenient method for diagnosing gate errors and also gives a good starting point for the constrained maximum likelihood estimation. * In the gate set, the first gate is generally selected to be the null gate. * The simulated errors are of three different types, representing coherent and incoherent gate errors as well as intrinsic SPAM errors.
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