From a485507e29115a8d9d7adc48a205a0082a8b6ada Mon Sep 17 00:00:00 2001 From: Wolfgang Bangerth Date: Sun, 8 Nov 2009 04:55:50 +0000 Subject: [PATCH] I liked the reference to the Copenhagen interpretation, so leave it in. git-svn-id: https://svn.dealii.org/trunk@20070 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/examples/step-36/doc/intro.dox | 2 +- 1 file changed, 1 insertion(+), 1 deletion(-) diff --git a/deal.II/examples/step-36/doc/intro.dox b/deal.II/examples/step-36/doc/intro.dox index 579cd909c9..5394c8e9cc 100644 --- a/deal.II/examples/step-36/doc/intro.dox +++ b/deal.II/examples/step-36/doc/intro.dox @@ -64,7 +64,7 @@ function $\Psi(\mathbf x)$ that satisfies a relation of the As a consequence, this particle can only exist in a certain number of eigenstates that correspond to the energy eigenvalues $\varepsilon_\ell$ admitted as solutions of this equation. The -orthodox interpretation of quantum mechanics posits that, if a +orthodox (Copenhagen) interpretation of quantum mechanics posits that, if a particle has energy $\varepsilon_\ell$ then the probability of finding it at location $\mathbf x$ is proportional to $|\Psi_\ell(\mathbf x)|^2$ where $\Psi_\ell$ is the eigenfunction that corresponds to this -- 2.39.5