Fig. 4

The frequency histogram statistics show the optimal Lagrangian multipliers \(\lambda ^{*}\) in all benchmark experiments. Where the Helmholtz equation contains \(\lambda ^{*}_{1}\), the Burgers equation contains \(\lambda ^{*}_{1},\lambda ^{*}_{2}\), the Black-Scholes equation contains \(\lambda ^{*}_{1},\lambda ^{*}_{2},\lambda ^{*}_{3}\), and the Klein-Gordon equation contains \(\lambda ^{*}_{1},\lambda ^{*}_{2},\lambda ^{*}_{3}\).