Reduced Density Matrices
A reduced density matrix is obtained by summing the unobserved subsystem’s matching bra and ket indices. It predicts measurements on the retained subsystem without selecting a remote outcome. Reduced density operators explains the full structure; here we focus on reading a matrix in a declared product basis.
Helpful background. Partial trace gives the dyad rule; density operators explains matrix entries and positivity.
Contracting the Unobserved Index
Section titled “Contracting the Unobserved Index”With rows and columns ordered as ,
For two qubits in the order , this reads
The index is the same on the bra and ket sides of every retained term. Do not sum all entries of a block or average by dividing by the subsystem dimension.
For example, gives , whereas tracing out gives .
Checking the Local Prediction
Section titled “Checking the Local Prediction”For every bounded local observable ,
In the example, in either calculation. The result remains positive with unit trace. It is the marginal state, not a state conditioned on a particular outcome.
Quick Check
Section titled “Quick Check”For that diagonal example, condition on a computational-basis result . Find its probability and the conditional state of , and compare it with .
Solution
The retained weights are for and for , so . Normalizing them gives , different from the marginal . Averaging all conditional states with their outcome probabilities recovers the marginal.
References
Section titled “References”- M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information, 10th anniversary ed., Cambridge University Press, 2010, sec. 2.4.3.
- J. Watrous, The Theory of Quantum Information, Cambridge University Press, 2018, ch. 2. Author’s manuscript.