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Photon assisted tunneling:

$$I_{p}(V_0,\alpha) = \sum_{n=-\infty}^{+\infty} J_n^2(\alpha) \cdot I_{dc}(V_0 + n\hbar \omega / e)$$

Components of $Y_{mm\prime} = G_{mm\prime} + i B_{mm\prime}$

$$G_{mm\prime} = \frac{e}{2 \hbar \omega_{m\prime}} \cdot \;\sum_{n,n\prime=-\infty}^{\infty} J_n(\alpha) J_{n\prime}(\alpha) \delta_{m-m\prime, n\prime-n} \left\{ \left[ I_{dc}(V_0+n\prime \hbar \omega /e + \hbar \omega_{m\prime}/e) - I_{dc}(V_0 + n\prime \hbar \omega/e) \right] + \left[ I_{dc}(V_0 + n\hbar \omega/e) - I_{dc}(V_0 + n \hbar \omega/e - \hbar \omega_{m\prime}/e) \right] \right\}$$ $$B_{mm\prime} = \frac{e}{2 \hbar \omega_{m\prime}} \cdot \sum_{n,n\prime=-\infty}^{\infty} J_n(\alpha) J_{n\prime}(\alpha) \delta_{m-m\prime, n\prime-n} \left\{ \left[ I_{kk}(V_0+n\prime \hbar \omega /e + \hbar \omega_{m\prime}/e) - I_{kk}(V_0 + n\prime \hbar \omega/e) \right] - \left[ I_{kk}(V_0 + n\hbar \omega/e) - I_{kk}(V_0 + n \hbar \omega/e - \hbar \omega_{m\prime}/e) \right] \right\}$$

$\omega_m = m \cdot \omega + \omega_0$

$\omega$ - LO rate, $\omega_0$ - IF rate, $\omega_m$ - Signal rate

Augmented

$$Y'_{mm} = \begin{bmatrix} Y_{11} + Y_{S} & Y_{10} & Y_{1-1} \\\ Y_{01} & Y_{00} + Y_L & Y_{0-1} \\\ Y_{-11} & Y_{-10} & Y_{-1-1}+Y_I \\\ \end{bmatrix}$$

$Y_{IF} = 1/Z'_{00}$

All there formulas from Tucker & Feldman theory

For I-V curve analysis used RespFnFromIVData from QMix https://github.com/garrettj403/QMix

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