Manuscript Em03-E@1 · Em03-E-v1.tex · section · c4b07e6a

E6: entropy trajectories and reference information

E6: entropy trajectories and reference information · lines 1776–1786

Let

H_{i} = - n = 0 \sum^{J_{i}} w_{i, n} lo g_{2} w_{i, n}, h_{η} = h_{2} ((1 + η) /2) .

The entropy calculations use the same dynamics as the channel and recovery calculations.

Displayed formulas in this passage

unlabeled · line 1780
$H_{i} = - n = 0 \sum^{J_{i}} w_{i, n} lo g_{2} w_{i, n}, h_{η} = h_{2} ((1 + η) /2) .$