#! /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