Abstract
We describe a simple method for certifying that an experimental device prepares a desired quantum state . Our method is applicable to any pure state , and it provides an estimate of the fidelity between and the actual (arbitrary) state in the lab, up to a constant additive error. The method requires measuring only a constant number of Pauli expectation values, selected at random according to an importance-weighting rule. Our method is faster than full tomography by a factor of , the dimension of the state space, and extends easily and naturally to quantum channels.
- Received 30 April 2011
DOI:https://doi.org/10.1103/PhysRevLett.106.230501
© 2011 American Physical Society