Equation:
\documentclass[12pt]{article}
\usepackage{mathtools}
\begin{document}
\begin{eqnarray}
\langle\pi_n|\hat{H}^{ab}|\pi_m\rangle & =& \Delta_{nm} g\int d^3x|\Psi_p(x-r_m)|^2\left\{|\phi_0(x)|^2+
\sum_{q=1}^{N}\left[\hat{b}_q\left(a\phi_0^*(x)-a\phi_0(x)\right)\right.\right.\\
& & +\left.\left. \phi*a*a*a-\phi^*_0(x)v^*_q(x)\right]\right\}
\end{eqnarray}
\end{document}
The third bracket at the end of the equation is of different size than the earlier bracket used in the first line.
