VAMPIRE
Auto-Correlation
Z-Gradient
SHG
\(\frac{dS_{mk}}{dE_n^*} = 0\)
\(\frac{dS_{mk}}{dE_n} = D_{kn}\left(A_{mk}+A_{mk}'+E_k\cdot e^{-i\tau_m\omega_n}\cdot(e^{-i\tau_0\omega_n} + e^{i\phi_n})\right)\)
THG
\(\frac{dS_{mk}}{dE_n^*} = 0\)
\(\frac{dS_{mk}}{dE_n} = D_{kn}(A_{mk}+A_{mk}')\cdot\left(A_{mk}+A_{mk}'+2E_k\cdot e^{-i\tau_m\omega_n}\cdot(e^{-i\tau_0\omega_n} + e^{i\phi_n})\right)\)
PG
\(\frac{dS_{mk}}{dE_n^*} = D_{nk}E_k(A_{mk}+A_{mk}')\cdot e^{i\tau_m\omega_n}(e^{i\tau_0\omega_n}+e^{-i\phi_n})\)
\(\frac{dS_{mk}}{dE_n} = D_{kn}(A_{mk}+A_{mk}')^*\cdot\left(A_{mk}+A_{mk}'+E_k e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n}+e^{i\phi_n})\right)\)
SD
\(\frac{dS_{mk}}{dE_n^*} = 2 D_{nk}E_k (A_{mk}+A_{mk}')^*\cdot e^{i\tau_m\omega_n}(e^{i\tau_0\omega_n}+e^{-i\phi_n})\)
\(\frac{dS_{mk}}{dE_n} = D_{kn}\left((A_{mk}+A_{mk}')^*\right)^2\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)
\(\frac{dS_{mk}}{dE_n} = D_{kn}(A_{mk}+A_{mk}')^{n-2}\cdot\left(A_{mk}+A_{mk}'+(n-1)E_k\cdot e^{-i\tau_m\omega_n}\cdot(e^{-i\tau_0\omega_n} + e^{i\phi_n})\right)\)
Z-Pseudo-Hessian
SHG
\(V_{zz}=0\)
THG
\(V_{zz}=0\)
PG
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = D_{nk}D_{kp}\cdot\left((E_k'+A_{mk}'')^*\cdot e^{-i\tau_m\omega_p}(e^{-i\tau_0\omega_p} + e^{i\phi_p}) + E_k^*\cdot e^{i\tau_m\omega_n}(e^{-i\tau_0\omega_n} + e^{i\phi_n})^*e^{-i\tau_m\omega_p}(e^{-i\tau_0\omega_p} + e^{i\phi_p})\right)\)
\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = D_{pk}D_{kn}\cdot\left((E_k'+A_{mk}'')^*\cdot e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n} + e^{i\phi_n}) + E_k^*\cdot e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n} + e^{i\phi_n}) e^{i\tau_m\omega_p}(e^{-i\tau_0\omega_p} + e^{i\phi_p})^*\right)\)
SD
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = D_{nk}D_{kp}\cdot 2(E_k'+A_{mk}'')e^{i\tau_m\omega_p}(e^{-i\tau_0\omega_p} + e^{i\phi_p})^*\)
\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = D_{pk}D_{kn}\cdot 2(E_k'+A_{mk}'')e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n} + e^{i\phi_n})\)
nth-HG
\(V_{zz} = 0\)
Cross-Correlation
Z-Gradient (with respect to pulse)
Same for all nonlinear methods
\(\frac{dS_{mk}}{dE_n^*} = 0\)
\(\frac{dS_{mk}}{dE_n} = D_{kn}G_{mk}\)
Z-Gradient (with respect to gate-pulse)
SHG
\(\frac{dS_{mk}}{dA_n^*} = 0\)
\(\frac{dS_{mk}}{dA_n} = D_{kn}E_k e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n}+e^{i\phi_n})\)
THG
\(\frac{dS_{mk}}{dA_n^*} = 0\)
\(\frac{dS_{mk}}{dA_n} = 2 D_{kn}E_k (A_{mk}+A_{mk}')\cdot e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n}+e^{i\phi_n})\)
PG
\(\frac{dS_{mk}}{dA_n^*} = D_{nk}E_k(A_{mk}+A_{mk}')\cdot e^{i\tau_m\omega_n}(e^{i\tau_0\omega_n}+e^{-i\phi_n})\)
\(\frac{dS_{mk}}{dA_n} = D_{kn}E_k(A_{mk}+A_{mk}')^*\cdot e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n}+e^{i\phi_n})\)
SD
\(\frac{dS_{mk}}{dA_n^*} = 2 D_{nk}E_k (A_{mk}+A_{mk}')^*\cdot e^{i\tau_m\omega_n}(e^{i\tau_0\omega_n}+e^{-i\phi_n})\)
\(\frac{dS_{mk}}{dA_n} = 0\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)
\(\frac{dS_{mk}}{dE_n} = (n-1) D_{kn}E_k (A_{mk}+A_{mk}')^{n-2}\cdot e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n}+e^{i\phi_n})\)
Z-Pseudo-Hessian (with respect to pulse)
Same for all nonlinear methods
\(V_{zz} = 0\)
Z-Pseudo-Hessian (with respect to gate-pulse)
SHG
\(V_{zz}=0\)
THG
\(V_{zz}=0\)
PG
\(\frac{d}{dA_p}\left(\frac{dS_{mk}}{dA_n}\right)^* = D_{nk}D_{kp}\cdot e^{i\tau_m\omega_n}(e^{-i\tau_0\omega_n} + e^{i\phi_n})^* e^{-i\tau_m\omega_p}(e^{-i\tau_0\omega_p} + e^{i\phi_p})\cdot E_k^*\)
\(\frac{d}{dA_p^*}\left(\frac{dS_{mk}}{dA_n^*}\right)^* = D_{kn}D_{pk}\cdot e^{-i\tau_m\omega_n}(e^{-i\tau_0\omega_n} + e^{i\phi_n})e^{i\tau_m\omega_p}(e^{-i\tau_0\omega_p} + e^{i\phi_p})^*\cdot E_k^*\)
SD
\(V_{zz}=0\)
nth-HG
\(V_{zz} = 0\)