#! /bin/sh /usr/share/dpatch/dpatch-run ## 100-fix-isajet-manual-corruption.dpatch by <kmccarty@debian.org> ## ## All lines beginning with `## DP:' are a description of the patch. ## DP: Fix corruption in LaTeX source to the Isajet manual. ## DP: (Replacement text obtained from a PS version of the manual on the web.) @DPATCH@ diff -urNad cernlib-2005.05.09/src/mclibs/isajet/doc/physics.doc /tmp/dpep.tlmeFD/cernlib-2005.05.09/src/mclibs/isajet/doc/physics.doc --- cernlib-2005.05.09/src/mclibs/isajet/doc/physics.doc 2001-10-08 10:03:08.000000000 -0400 +++ /tmp/dpep.tlmeFD/cernlib-2005.05.09/src/mclibs/isajet/doc/physics.doc 2005-06-08 16:12:37.814042242 -0400 @@ -122,7 +122,7 @@ $W/Z$ decay. These were calculated using FORM 1.1 by J.~Vermaseren. The process $g + t \to W + b$ is {\it not} included. Both $g + b \to W^- + t$ and $g + \bar t \to W^- + \bar b$ of course give the same $W^- + t -+\BARB_FINALSTATEAFTERQCDEVOLUTION ++\bar b$ final state after QCD evolution. While the latter process is needed to describe the $m_t = 0$(!) mass singularity for $q_t \gg m_t$, it has a pole in the physical region at low $q_t$ from on-shell $t \to W + b$ decays. There is no obvious way to avoid this without