TY - JOUR
T1 - Optimal error regions for quantum state estimation
AU - Shang, Jiangwei
AU - Ng, Hui Khoon
AU - Sehrawat, Arun
AU - Li, Xikun
AU - Englert, Berthold Georg
PY - 2013/12
Y1 - 2013/12
N2 - An estimator is a state that represents one's best guess of the actual state of the quantum system for the given data. Such estimators are points in the state space. To be statistically meaningful, they have to be endowed with error regions, the generalization of error bars beyond one dimension. As opposed to standard ad hoc constructions of error regions, we introduce the maximum-likelihood region - the region of largest likelihood among all regions of the same size - as the natural counterpart of the popular maximum-likelihood estimator. Here, the size of a region is its prior probability. A related concept is the smallest credible region - the smallest region with pre-chosen posterior probability. In both cases, the optimal error region has constant likelihood on its boundary. This surprisingly simple characterization permits concise reporting of the error regions, even in high-dimensional problems. For illustration, we identify optimal error regions for single-qubit and two-qubit states from computer-generated data that simulate incomplete tomography with few measured copies.
AB - An estimator is a state that represents one's best guess of the actual state of the quantum system for the given data. Such estimators are points in the state space. To be statistically meaningful, they have to be endowed with error regions, the generalization of error bars beyond one dimension. As opposed to standard ad hoc constructions of error regions, we introduce the maximum-likelihood region - the region of largest likelihood among all regions of the same size - as the natural counterpart of the popular maximum-likelihood estimator. Here, the size of a region is its prior probability. A related concept is the smallest credible region - the smallest region with pre-chosen posterior probability. In both cases, the optimal error region has constant likelihood on its boundary. This surprisingly simple characterization permits concise reporting of the error regions, even in high-dimensional problems. For illustration, we identify optimal error regions for single-qubit and two-qubit states from computer-generated data that simulate incomplete tomography with few measured copies.
UR - http://www.scopus.com/inward/record.url?scp=84891749207&partnerID=8YFLogxK
U2 - 10.1088/1367-2630/15/12/123026
DO - 10.1088/1367-2630/15/12/123026
M3 - Article
AN - SCOPUS:84891749207
SN - 1367-2630
VL - 15
JO - New Journal of Physics
JF - New Journal of Physics
M1 - 123026
ER -