From d046e13265dd9864e5a00089e88e7aaa80394210 Mon Sep 17 00:00:00 2001 From: Wolfgang Bangerth Date: Thu, 30 Jul 2009 13:01:51 +0000 Subject: [PATCH] Minor text edit. git-svn-id: https://svn.dealii.org/trunk@19135 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/examples/step-36/doc/intro.dox | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/deal.II/examples/step-36/doc/intro.dox b/deal.II/examples/step-36/doc/intro.dox index 1df6e81ec8..32fb3ea090 100644 --- a/deal.II/examples/step-36/doc/intro.dox +++ b/deal.II/examples/step-36/doc/intro.dox @@ -52,9 +52,9 @@ for linear algebra contents. The basic equation of stationary quantum mechanics is the Schrödinger equation which models the motion of particles in an -external potential $V(\mathbf x)$ as if it were governed a wave +external potential $V(\mathbf x)$. The particle is described by a wave function $\Psi(\mathbf x)$ that satisfies a relation of the -(non-dimensionalized ) form +(non-dimensionalized) form @f{align*} [-\Delta + V(\mathbf x)] \Psi(\mathbf x) &= \varepsilon \Psi(\mathbf x) \qquad &&\text{in}\ \Omega\quad, \\ \Psi &= 0 &&\text{on}\ \partial\Omega\quad. -- 2.39.5