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Table 6 Comparison of time-averaged mixing coefficients under stationary conditions

From: Sequential convex combinations of multiple adaptive lattice filters in cognitive radio channel identification

R-CFLF  
\(\bar {v}^{1}=0.219662\) \(\bar {v}^{2}=0.329039\) \(\bar {v}^{3}=0.224948\) \(\bar {v}^{4}=0.226642\)
D-CFLF  
\(\bar {v}^{1}_{1}=0.250000\) \(\bar {v}^{2}_{1}=0.250000\) \(\bar {v}^{3}_{1}=0.250000\) \(\bar {v}^{4}_{1}=0.250000\)
\(\bar {v}^{1}_{2}=0.260383\) \(\bar {v}^{2}_{2}=0.245273\) \(\bar {v}^{3}_{2}=0.243011\) \(\bar {v}^{4}_{2}=0.248331\)
\(\bar {v}^{1}_{3}=0.260950\) \(\bar {v}^{2}_{3}=0.238969\) \(\bar {v}^{3}_{3}=0.240371\) \(\bar {v}^{4}_{3}=0.256708\)
\(\bar {v}^{1}_{4}=0.259955\) \(\bar {v}^{2}_{4}=0.238969\) \(\bar {v}^{3}_{4}=0.240596\) \(\bar {v}^{4}_{4}=0.259483\)
\(\bar {v}^{1}_{5}=0.259482\) \(\bar {v}^{2}_{5}=0.235899\) \(\bar {v}^{3}_{5}=0.240934\) \(\bar {v}^{4}_{5}=0.260747\)
\(\bar {v}^{1}_{6}=0.258075\) \(\bar {v}^{2}_{6}=0.235125\) \(\bar {v}^{3}_{6}=0.241462\) \(\bar {v}^{4}_{6}=0.262336\)
\(\bar {v}^{1}_{7}=0.256902\) \(\bar {v}^{2}_{7}=0.234466\) \(\bar {v}^{3}_{7}=0.242221\) \(\bar {v}^{4}_{7}=0.263409\)
\(\bar {v}^{1}_{8}=0.307697\) \(\bar {v}^{2}_{8}=0.137990\) \(\bar {v}^{3}_{8}=0.267800\) \(\bar {v}^{4}_{8}=0.283511\)
\(\bar {v}^{1}_{9}=0.300305\) \(\bar {v}^{2}_{9}=0.146743\) \(\bar {v}^{3}_{9}=0.267666\) \(\bar {v}^{4}_{9}=0.282285\)
\(\bar {v}^{1}_{10}=0.294155\) \(\bar {v}^{2}_{10}=0.155295\) \(\bar {v}^{3}_{10}=0.267576\) \(\bar {v}^{4}_{10}=0.279972\)
\(\bar {v}^{1}_{11}=0.287647\) \(\bar {v}^{2}_{11}=0.167800\) \(\bar {v}^{3}_{11}=0.266095\) \(\bar {v}^{4}_{11}=0.275457\)
\(\bar {v}^{1}_{12}=0.283007\) \(\bar {v}^{2}_{12}=0.180514\) \(\bar {v}^{3}_{12}=0.263361\) \(\bar {v}^{4}_{12}=0.270116\)
M-CLMS  
\(\bar {v}^{1}=0.194679\) \(\bar {v}^{2}=0.430737\) \(\bar {v}^{3}=0.185233\) \(\bar {v}^{4}=0.186599\)
D-CLMS  
\(\bar {v}^{1}_{1}=0.439073\) \(\bar {v}^{2}_{1}=0.560926\)  
\(\bar {v}^{1}_{2}=0.439087\) \(\bar {v}^{2}_{2}=0.560991\)  
\(\bar {v}^{1}_{3}=0.438953\) \(\bar {v}^{2}_{3}=0.561046\)  
\(\bar {v}^{1}_{4}=0.438959\) \(\bar {v}^{2}_{4}=0.560403\)  
\(\bar {v}^{1}_{5}=0.438893\) \(\bar {v}^{2}_{5}=0.561116\)  
\(\bar {v}^{1}_{6}=0.439248\) \(\bar {v}^{2}_{6}=0.560751\)  
\(\bar {v}^{1}_{7}=0.437971\) \(\bar {v}^{2}_{7}=0.562028\)  
\(\bar {v}^{1}_{8}=0.436686\) \(\bar {v}^{2}_{6}=0.563313\)  
\(\bar {v}^{1}_{9}=0.437216\) \(\bar {v}^{2}_{9}=0.562783\)  
\(\bar {v}^{1}_{10}=0.436428\) \(\bar {v}^{2}_{10}=0.563471\)  
\(\bar {v}^{1}_{11}=0.437432\) \(\bar {v}^{2}_{11}=0.562567\)  
\(\bar {v}^{1}_{12}=0.436643\) \(\bar {v}^{2}_{12}=0.563356\)