How do I get only one equation number displayed in an
align*
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\begin{align*}\end{align*}
align*
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\begin{align*}\end{align*}
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equation
environment and within this an aligned
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\begin{equation}\begin{align}{E}_{PD}\ \left(t \right) =& \!\left[ {T}_o{J}_o\left({{m}_{RF}} \right) + j{J}_1\left({{m}_{RF}} \right){e}^{j\frac{1}{2}{\beta }_2L\omega _{RF}^2} \right.\\ & \times \left({{e}^{j{\omega }_{RF}t} + {e}^{ - j{\omega }_{RF}t}} \right) \\ & \!-\! \left. {J}_2\left({{m}_{RF}} \right){e}^{j2{\beta }_2L\omega _{RF}^2}\!\left({{e}^{j2{\omega }_{RF}t} \!+\! {e}^{ - j2{\omega }_{RF}t}} \!\right) \!\right] e ^{j{\omega }_ot}\\ & + {T}_o{J}_o\left({{m}_{RF}} \right){e}^{j\frac{1}{2}{\beta }_2L\omega _{IF}^2}\left({m}_ + \cdot {e}^{j{\omega }_{IF}t} + {m}_ - \right.\\ & \cdot \left. {e}^{ - j{\omega }_{IF}t} \right){e}^{j{\omega }_ot} + j{J}_1\left({{m}_{RF}} \right){e}^{j\frac{1}{2}{\beta }_2L{{\left({{\omega }_{RF} + {\omega }_{IF}} \right)}}^2}\\ & \times \left({{m}_ + {e}^{j\left({{\omega }_{RF} + {\omega }_{IF}} \right)t} + {m}_ - {e}^{ - j\left({{\omega }_{RF} + {\omega }_{IF}} \right)t}} \right){e}^{j{\omega }_ot} \\ & + j{J}_1\left({{m}_{RF}} \right){e}^{j\frac{1}{2}{\beta }_2L{{\left({{\omega }_{RF} - {\omega }_{IF}} \right)}}^2}\\ &\!\times\! \left({{m}_ - \cdot {e}^{j\left({{\omega }_{RF} \!-\! {\omega }_{IF}} \right)t} \!+\! {m}_ + \cdot {e}^{ - j\left({{\omega }_{RF} \!-\! {\omega }_{IF}} \right)t}} \right){e}^{j{\omega }_ot} \\ & - {J}_2\left({{m}_{RF}} \right){e}^{j\frac{1}{2}{\beta }_2L{{\left({2{\omega }_{RF} + {\omega }_{IF}} \right)}}^2}\\ & \times \left({{m}_ + \cdot {e}^{j\left({2{\omega }_{RF} + {\omega }_{IF}} \right)t} + {m}_ - \cdot {e}^{ - j\left({2{\omega }_{RF} + {\omega }_{IF}} \right)t}} \right)\\ & \times {e}^{j{\omega }_ot} - {J}_2\left({{m}_{RF}} \right){e}^{j\frac{1}{2}{\beta }_2L{{\left({2{\omega }_{RF} - {\omega }_{IF}} \right)}}^2}\\ & \!\times\! \left({{m}_ - \cdot {e}^{j\!\left({2{\omega }_{RF} \!-\! {\omega }_{IF}} \!\right)t} \!+\! {m}_ + \cdot {e}^{ - j\!\left({2{\omega }_{RF} \!-\! {\omega }_{IF}} \!\right)t}} \!\right){e}^{j{\omega }_ot}\end{align}\end{equation}\label{poc_E_PD_t}
aligned
instead of align
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\begin{table}[h]\caption{Analytical Terms of the Photocurrent Amplitude at mmW Band}\centering\begin{tabular}{p{1cm}p{1cm}p{9cm}}\hline\hline\centering L&$\centering T_0$& \centering\arraybackslash $i_{RF}(2\omega_{RF}-\omega_{IF})$\\\hline\[\text{0}\] & \[\text{1}\] & \begin{equation} 0 \label{poc_eq_10} \end{equation}\\\[\text{L}\] & \[\text{1}\] & \begin{equation}\begin{aligned}&2 \Re P_0 m_{AM}\left(\frac{m_{RF}}{2}\right)^2 sin^2 \Theta& \cdot \left[\sqrt{1+\alpha^2}cos(\Theta - atan \alpha) + j\alpha \frac{\kappa P_0}{\omega_{IF}}sin\Theta \right] \label{poc_eq_11}\end{aligned}\end{equation}\\\[\text{L}\] & \[\text{0}\] &\begin{equation}\begin{aligned}&\Re P_0 m_{AM}\left(\frac{m_{RF}}{2}\right)^2& \cdot \left[\sqrt{1+\alpha^2}cos(\Theta - atan \alpha) + j\alpha \frac{\kappa P_0}{\omega_{IF}}sin\Theta \right] \label{poc_eq_12}\end{aligned}\end{equation}\\\hline\hline\end{tabular}\label{poc_Table_1}
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And: Currently, Packt sells ebooks for $4.99 each if you buy 5 of their over 1000 ebooks. If you choose only a single one, $9.99. How about combining 3 LaTeX books with Python, gnuplot, mathplotlib, Matlab, ChatGPT or other AI books? Epub and PDF. Bundle (3 books, add more for higher discount): https://packt.link/MDH5p