 enter npoints,number_propagators,rank,scaloop,muscale
     
 scaloop= 1 -> looptools 1-loop 
 scaloop= 2 -> avh 1-loop (massive with complex masses)
 scaloop= 3 -> qcdloop   1-loop (Ellis and Zanderighi)
 muscale (dimension of energy) is the scale
 for the 1-loop integrals
     
  
------------------------------------------------------------------------
|              You are using CutTools - Version 1.7.0                  |
|              Authors: G. Ossola, C. Papadopoulos, R. Pittau          |
|              Published in JHEP 0803:042,2008                         |
|              http://www.ugr.es/~pittau/CutTools                      |
|                                                                      |
|              Internal mproutines detected in CutTools                |
------------------------------------------------------------------------
   
########################################################################
#                                                                      #
#                      You are using OneLOop-2.2                       #
#                                                                      #
# for the evaluation of 1-loop scalar 1-, 2-, 3- and 4-point functions #
#                                                                      #
# author: Andreas van Hameren <hamerenREMOVETHIS@ifj.edu.pl>           #
#   date: 04-07-2011                                                   #
#                                                                      #
# Please cite                                                          #
#    A. van Hameren,                                                   #
#      Comput.Phys.Commun. 182 (2011) 2427-2438, arXiv:1007.4716       #
#    A. van Hameren, C.G. Papadopoulos and R. Pittau,                  #
#      JHEP 0909:106,2009, arXiv:0903.4665                             #
# in publications with results obtained with the help of this program. #
#                                                                      #
########################################################################
########################################################################
#                                                                      #
#          You are using OneLOop in multiple precision                 #
#                                                                      #
#             obtained by R. Pittau (pittau@ugr.es)                    #
#             from the original OneLOop-2.2 package                    #
#                                                                      #
#                 Internal mproutines detected.                        #
#                                                                      #
########################################################################
                
   iter=            1
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  77834.779048846380     ,  210665.04498575686     )
  coeff of 1/eps   pole amp(1)= ( 1.00698684946110006E-008,-9.63190028785021844E-009)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  84024.357080695365     ,  210665.04498577159     )
                            R1= ( -6189.5780318489878     ,-1.47151645535359441E-008)
                        stable= T
                
                
   iter=            2
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  2.9365797108784761     , -45.243908938505136     )
  coeff of 1/eps   pole amp(1)= ( 2.90873325425877738E-010, 1.68615741497265182E-010)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  156.38227548424499     , -45.243908950897072     )
                            R1= ( -153.44569577336651     , 1.23919332795097151E-008)
                        stable= T
                
                
   iter=            3
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -23391.672907069951     ,  37974.591875738479     )
  coeff of 1/eps   pole amp(1)= ( 3.02406988339498639E-010,-4.73282950660557437E-009)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -29361.736096918463     ,  37974.591875733044     )
                            R1= (  5970.0631898485099     , 5.43580827641609882E-009)
                        stable= T
                
                
   iter=            4
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  11.220394488085688     ,  13.650693522230842     )
  coeff of 1/eps   pole amp(1)= (-4.14643250290502863E-011,-6.45303903123147950E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -35.361989112683091     ,  13.650693522177285     )
                            R1= (  46.582383600768779     , 5.35576916149695060E-011)
                        stable= T
                
                
   iter=            5
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  4722.7174106680477     ,  307.17654231945698     )
  coeff of 1/eps   pole amp(1)= ( 2.38209452163573587E-011,-3.77664923680101279E-011)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  4665.1112448673684     ,  307.17654232023921     )
                            R1= (  57.606165800679520     ,-7.82225281770187978E-010)
                        stable= T
                
                
   iter=            6
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -720.46341258793859     ,  1043.5514515303948     )
  coeff of 1/eps   pole amp(1)= (-4.83737494505476207E-011,-3.88885252841867230E-011)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -2458.1652455151611     ,  1043.5514515301832     )
                            R1= (  1737.7018329272225     , 2.11706996378069345E-010)
                        stable= T
                
                
   iter=            7
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -90.265229666506741     , -89.382756371052409     )
  coeff of 1/eps   pole amp(1)= (-8.91011708858968632E-011, 1.53835430595252475E-010)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -105.56795311808551     , -89.382756373240284     )
                            R1= (  15.302723451578764     , 2.18787903349948448E-009)
                        stable= T
                
                
   iter=            8
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  11.149727586575281     ,  53.536637181298133     )
  coeff of 1/eps   pole amp(1)= ( 1.07517439396076497E-010, 1.52877427812376368E-010)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  120.87961239913756     ,  53.536637178303451     )
                            R1= ( -109.72988481256228     , 2.99468503328625965E-009)
                        stable= T
                
                
   iter=            9
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -57.396503211365655     ,  4715.9796061225652     )
  coeff of 1/eps   pole amp(1)= ( 2.92300239568277220E-010,-1.01753920750402322E-009)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  179.15280531062632     ,  4715.9796061304451     )
                            R1= ( -236.54930852199197     ,-7.87985260861101577E-009)
                        stable= T
                
                
   iter=           10
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -2271.8198274458960     ,  834.53073338254819     )
  coeff of 1/eps   pole amp(1)= ( 4.19716172928019660E-009, 2.98086882723809297E-009)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -2122.3230995799731     ,  834.53073338215177     )
                            R1= ( -149.49672786592291     , 3.96480892561612605E-010)
                        stable= T
                
 n_tot =   10.000000000000000     
 n_mp  =   0.0000000000000000     
 n_disc=           0
