Alternative Equation Formats

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MathML

\begin{array}{rcl} {\hat{J}}_{1 k} (t; z_{0}) & = & \dot{m} [{\hat{F}}_{1} (t; z_{0})] \exp [- {\hat{Λ}}_{1} (t; z_{0})] \sum_{i = 1}^{n} A_{k i} {\int_{0}^{t} \frac{\exp ({\hat{β}}^{'} z_{0})}{S_{2}^{(0)} (\hat{β}, u)} w_{i} (u) d {\hat{M}}_{i}^{1} (u) \\ + {\hat{h}}^{'} (t; z_{0}) {\hat{Ω}}^{- 1} ({\hat{η}}_{i} + {\hat{ψ}}_{i}) + \int_{0}^{\infty} \frac{\hat{v} (u, t, z_{0})}{\hat{π} (u)} d {\hat{M}}_{i}^{c} (u)} \end{array}

Math Rendered as SVG

Math as LaTeX Source

\begin{eqnarray*} \hat{J}_{1k}(t;\bm {z}_0) & = & \dot{m}[\hat{F}_1(t;\mb{z}_0)]\exp [- \hat{\Lambda }_1(t;\mb{z}_0)] \sum _{i=1}^ n A_{ki} \biggl \{ \int _0^ t \frac{\exp (\hat{\bbeta }'\bm {z}_0)}{S_2^{(0)}(\hat{\bbeta },u)} w_ i(u) d\hat{M}^1_ i(u) \\ & & + ~ \hat{\bm {h}}'(t;\bm {z}_0) \hat{\bOmega }^{-1}(\hat{\bm {\eta }}_ i + \hat{\bpsi }_ i) + \int _0^\infty \frac{\hat{\bm {v}}(u,t,\bm {z}_0)}{\hat{\pi }(u)} d\hat{M}_ i^ c(u) \biggr \} \end{eqnarray*}