Alternative Equation Formats

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MathML

\begin{aligned} S_{t 1} & = \sum_{j = 1}^{r_{M}} ϕ_{j}^{(E)} \\ S_{t 2} & = \sum_{j = 1}^{r_{M}} ϕ_{j}^{(E)} ω_{* j} \\ S_{t 3} & = \sum_{j = 1}^{r_{M}} {(ϕ_{j}^{(E)})}^{2} \\ S_{t 4} & = \sum_{j = 1}^{r_{M}} {(ϕ_{j}^{(E)})}^{2} ω_{* j} \end{aligned}

MathML rendered with MathJax

\begin{aligned} S_{t 1} & = \sum_{j = 1}^{r_{M}} ϕ_{j}^{(E)} \\ S_{t 2} & = \sum_{j = 1}^{r_{M}} ϕ_{j}^{(E)} ω_{* j} \\ S_{t 3} & = \sum_{j = 1}^{r_{M}} {(ϕ_{j}^{(E)})}^{2} \\ S_{t 4} & = \sum_{j = 1}^{r_{M}} {(ϕ_{j}^{(E)})}^{2} ω_{* j} \end{aligned}

Math as LaTeX Source

\begin{align*} S_{t1} & = \sum _{j=1}^{r_ M} \phi _ j^{(\mr{E})} \\ S_{t2} & = \sum _{j=1}^{r_ M} \phi _ j^{(\mr{E})} \omega _{*j} \\ S_{t3} & = \sum _{j=1}^{r_ M} \left( \phi _ j^{(\mr{E})} \right)^2 \\ S_{t4} & = \sum _{j=1}^{r_ M} \left( \phi _ j^{(\mr{E})} \right)^2 \omega _{*j} \end{align*}