Created by Valentin Hirschi on 2017-06-19 and last modified on 2019-10-02
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Recent revisions

529. By Rikkert Frederix on 2019-10-02

need to count the i_dipole_dead_counter twice in case of the
is_special when we're in the dead-zone.

528. By Rikkert Frederix on 2019-10-01

move the default MClow and MCdelta back to 10 and 20, respectively

527. By Rikkert Frederix on 2019-10-01

Use the *unconstrained* version of scale assignment

526. By Paolo Torrielli on 2019-09-11

added comments to the routine that computes deadzones

525. By Rikkert Frederix on 2019-08-27

Added a tiny cutoff in the computation of Qsq in Pythia. If below
cut-off (which is far below the shower cutoff) there won't be viable
scales: need to set Sudakov to zero.

524. By Rikkert Frederix on 2019-08-26

set the debug_verbose by default to .FALSE. (don't want the fort.9?
files). Also removed the -fbounds-check errors

523. By Rikkert Frederix on 2019-08-26

set the glrat(1:2) both to 0.5d0 in case they are 'ill-defined'

522. By Rikkert Frederix on 2019-08-13

fixes in MonteCarloCounter related to capping the maximum values of the
stopping scale and dipole masses (as returned by pythia and used in the
pysudakov() routines). Also fixed an issue with an undefined 'j' in the
xmasses2(i,j) arrays.

521. By Rikkert Frederix on 2019-08-08

Added the three sudakov files (for pythia8) using the three PDFmodes

520. By Rikkert Frederix on 2019-08-08

Added extra phase-space checks to make sure that the event before and after
clustering are consistent in Pythia. If outside of phase-space, return a scale
equal to zero (which should be interpreted in montecarlocounter as infinity).

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