Reconstruction of dynamic structures of experimental setups based on measurable experimental data only
Chen Tian-Yu1, Chen Yang1, Yang Hu-Jiang1, Xiao Jing-Hua1, †, Hu Gang2, ‡
       

(color online) (a) and (b) Parameters reconstructed with 2 different truncations M s (vertical lines) plotted against those reconstructed by M truncation adopted in Eq. (11). M > M ( M = 11 , Z M = ( θ ˙ , cos ( ω t ) , sin ( ω t ) , cos ( θ ) , sin ( θ ) , cos ( 2 θ ) , sin ( 2 θ ) , cos ( 3 θ ) , sin ( 3 θ ) , cos ( 6 θ ) , sin ( 6 θ ) ) , F = ( F 1 , F 2 , F 3 , F 4 , F 5 , F 6 , F 7 , F 8 , F 9 , F 10 , F 11 ) ) and M includes all M parameters of Eq. (11), all dots are around the diagonal line and all parameters not included in the M of Eq. (11) bases are nearly zero (red circles), justifying the sufficiency of truncation of Eq. (11). (b) The same as panel (a) with two terms of cos ( 2 θ ) , sin ( 2 θ ) in Eq. (11) deleted (M = 7, Z M = ( θ ˙ , cos ( ω t ) , sin ( ω t ) , cos ( θ ) , sin ( θ ) , cos ( 3 θ ) , sin ( 3 θ ) ) , F = ( F 1 , F2, F3, F4, F5, F6, F 7 ) . Dots distribute considerably away from the diagonal line, concluding such truncation of M = 7 not suitable.