Time-Domain-Ptychography
Auto-Correlation
Z-Gradient
SHG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = D_{kn}\cdot(A_{mk}' + B_n\cdot e^{-i\tau_m\omega_n} E_k)\)
THG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = D_{kn}\cdot(A_{mk}'^2 + 2B_n\cdot e^{-i\tau_m\omega_n} E_k A_{mk})\)
PG
\(\frac{dS_{mk}}{dE_n^*} = D_{nk} \cdot B_n^*\cdot e^{i\tau_m\omega_n} E_k A_{mk}\)\(\frac{dS_{mk}}{dE_n} = D_{kn} A_{mk}'^* \cdot (A_{mk}' + B_n\cdot e^{-i\tau_m\omega_n} E_k)\)
SD
\(\frac{dS_{mk}}{dE_n^*} = 2 D_{nk} B_n^*\cdot E_k A_{mk}'^* e^{i\tau_m\omega_n}\)\(\frac{dS_{mk}}{dE_n} = D_{kn} (A_{mk}'^*)^2\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = D_{kn}\cdot(A_{mk}'^{n-1} + (n-1)B_n\cdot e^{-i\tau_m\omega_n} E_k A_{mk}^{n-2})\)
Z-Pseudo-Hessian
SHG
\(V_{zz} = 0\)
THG
\(V_{zz} = 0\)
PG
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = D_{pk} D_{kn}\cdot \left( A_{mk}'^* B_p e^{-i\tau_m\omega_p} + E_k^* B_n^*B_p e^{i\tau_m\omega_n} e^{-i\tau_m\omega_p} \right)\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = D_{nk} D_{kp} \cdot \left( A_{mk}'^* B_n e^{-i\tau_m\omega_n} + E_k^* B_nB_p^* e^{i\tau_m\omega_p} e^{-i\tau_m\omega_n} \right)\)
SD
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = 2\cdot D_{pk}D_{kn} \cdot A_{mk}' B_p e^{-i\tau_m\omega_p}\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = 2\cdot D_{nk}D_{kp} \cdot A_{mk}' B_n e^{-i\tau_m\omega_n}\)
nth-HG
\(V_{zz} = 0\)
Cross-Correlation
Z-Gradient (with respect to pulse)
Same for all nonlinear methods
\(\frac{dS_{mk}}{dE_n^*} = 0\)
\(\frac{dS_{mk}}{dE_n} = D_{kn} G(A_{mk}')\)
Z-Gradient (with respect to gate-pulse)
\(\frac{dS_{mk}}{dE_n} = \frac{dS_{mk}}{dA_{mk}'}\frac{dA_{mk}'}{dE_n}\)
\(\frac{dS_{mk}}{dE_n^*} = \frac{dS_{mk}}{dA_{mk}'^*}\left(\frac{dA_{mk}'}{dE_n}\right)^*\)
SHG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = D_{kn} B_n\cdot E_k e^{-i\tau_m\omega_n}\)
THG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 2 \cdot D_{kn} B_n\cdot E_k A_{mk}' e^{-i\tau_m\omega_n}\)
PG
\(\frac{dS_{mk}}{dE_n^*} = D_{nk} \cdot B_n^*\cdot E_k A_{mk}' e^{i\tau_m\omega_n}\)\(\frac{dS_{mk}}{dE_n} = D_{kn} \cdot B_n\cdot E_k A_{mk}'^* e^{-i\tau_m\omega_n}\)
SD
\(\frac{dS_{mk}}{dE_n^*} = 2\cdot D_{nk} B_n^*\cdot E_k A_{mk}'^* e^{i\tau_m\omega_n}\)\(\frac{dS_{mk}}{dE_n} = 0\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = (n-1) \cdot D_{kn} B_n\cdot E_k \left(A_{mk}'\right)^{n-2} e^{-i\tau_m\omega_n}\)
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
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = D_{nk}D_{kp} E_k^* B_n^*B_p e^{i\tau_m\omega_n} e^{-i\tau_m\omega_p}\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = D_{kn}D_{pk} E_k^* B_nB_p^* e^{-i\tau_m\omega_n} e^{i\tau_m\omega_p}\)
SD
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = 0\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = 0\)
nth-HG
\(V_{zz} = 0\)
Interferometric Time-Domain-Ptychography
Auto-Correlation
Z-Gradient
SHG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 2D_{kn}(1+B_n\cdot e^{-i\tau_m\omega_n})\cdot (E_k + A_{mk}')\)
THG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 3D_{kn}(1+B_n\cdot e^{-i\tau_m\omega_n})\cdot (E_k + A_{mk}')^2\)
PG/SD
\(\frac{dS_{mk}}{dE_n^*} = D_{nk}(1+B_n^*\cdot e^{i\tau_m\omega_n})\cdot (E_k + A_{mk}')^2\)\(\frac{dS_{mk}}{dE_n} = 2D_{kn}(1+B_n\cdot e^{-i\tau_m\omega_n})\cdot |E_k + A_{mk}'|^2\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = n\cdot D_{kn}(1+B_n\cdot e^{-i\tau_m\omega_n})\cdot (E_k + A_{mk}')^{n-1}\)
Z-Pseudo-Hessian
SHG
\(V_{zz} = 0\)
THG
\(V_{zz} = 0\)
PG/SD
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = 2D_{nk}D_{kp} (E_k+A_{mk}')^* (1+B_n^*e^{i\tau_m\omega_n}) (1+B_p e^{-i\tau_m\omega_p})\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = 2D_{kn}D_{pk} (E_k+A_{mk}')^* (1+B_n e^{-i\tau_m\omega_n}) (1+B_p^*e^{i\tau_m\omega_p})\)
nth-HG
\(V_{zz} = 0\)
Cross-Correlation
Z-Gradient (with respect to pulse)
SHG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 2D_{kn}(E_k + A_{mk}')\)
THG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 3D_{kn} (E_k + A_{mk}')^2\)
PG/SD
\(\frac{dS_{mk}}{dE_n^*} = D_{nk}(E_k + A_{mk}')^2\)\(\frac{dS_{mk}}{dE_n} = 2D_{kn}|E_k + A_{mk}'|^2\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = n\cdot D_{kn} (E_k + A_{mk}')^{n-1}\)
Z-Gradient (with respect to gate-pulse)
SHG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 2D_{kn}B_n\cdot e^{-i\tau_m\omega_n}(E_k + A_{mk}')\)
THG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = 3D_{kn}B_n\cdot e^{-i\tau_m\omega_n}(E_k + A_{mk}')^2\)
PG/SD
\(\frac{dS_{mk}}{dE_n^*} = D_{nk}B_n^*\cdot e^{i\tau_m\omega_n}(E_k + A_{mk}')^2\)\(\frac{dS_{mk}}{dE_n} = 2D_{kn}B_n\cdot e^{-i\tau_m\omega_n}|E_k + A_{mk}'|^2\)
nth-HG
\(\frac{dS_{mk}}{dE_n^*} = 0\)\(\frac{dS_{mk}}{dE_n} = n\cdot D_{kn}B_n\cdot e^{-i\tau_m\omega_n}(E_k + A_{mk}')^{n-1}\)
Z-Pseudo-Hessian (with respect to pulse)
SHG
\(V_{zz} = 0\)
THG
\(V_{zz} = 0\)
PG/SD
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = 2D_{nk}D_{kp} (E_k+A_{mk}')^*\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = 2D_{kn}D_{pk} (E_k+A_{mk}')^*\)
nth-HG
\(V_{zz} = 0\)
Z-Pseudo-Hessian (with respect to gate-pulse)
SHG
\(V_{zz} = 0\)
THG
\(V_{zz} = 0\)
PG/SD
\(\frac{d}{dE_p}\left(\frac{dS_{mk}}{dE_n}\right)^* = 2D_{nk}D_{kp} (E_k+A_{mk}')^* B_n^*B_p e^{i\tau_m\omega_n}e^{-i\tau_m\omega_p}\)\(\frac{d}{dE_p^*}\left(\frac{dS_{mk}}{dE_n^*}\right)^* = 2D_{kn}D_{pk} (E_k+A_{mk}')^* B_nB_p^* e^{-i\tau_m\omega_n}e^{i\tau_m\omega_p}\)
nth-HG
\(V_{zz} = 0\)