\documentclass[24pt]{article} \pagestyle{empty} \Huge \begin{document} \mathchardef\mhyphen="2D % The imaginary unit \providecommand*{\iu}% {\ensuremath{{\rm i}}} \begin{eqnarray*} \exp \left(\iu{} L \Delta t \right) &=&Ê \exp \left(\iu{} L_{\rm T\mhyphen baro} \frac{\Delta t}{2} \right) \exp \left(\iu{} L_{\rm T\mhyphen part} \frac{\Delta t}{2} \right) \exp \left(\iu{} L_{\epsilon , 2} \frac{\Delta t}{2} \right) \exp \left(\iu{} L_{2}^{(2)} \frac{\Delta t}{2} \right) \\ &&\times \left[ \exp \left(\iu{} L_{2}^{(1)} \frac{\Delta t}{2n} \right) \exp \left(\iu{} L_{\epsilon , 1} \frac{\Delta t}{n} \right) \exp \left(\iu{} L_1 \frac{\Delta t}{n} \right) \exp \left(\iu{} L_{2}^{(1)} \frac{\Delta t}{2n} \right) \right]^n \\ &&\times \exp \left(\iu{} L_{2}^{(2)} \frac{\Delta t}{2} \right) \exp \left(\iu{} L_{\epsilon , 2} \frac{\Delta t}{2} \right) \exp \left(\iu{} L_{\rm T\mhyphen part} \frac{\Delta t}{2} \right) \exp \left(\iu{} L_{\rm T\mhyphen baro} \frac{\Delta t}{2} \right) \\ &&+ \mathcal{O} \left(\Delta t^3 \right) \end{eqnarray*} \end{document}