 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)= (  53383957.821603358     ,  126986265.20322932     )
  coeff of 1/eps   pole amp(1)= (-1.83719203050713986E-006,-1.19366438964925456E-006)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  431278153.45692199     ,  126986265.19815829     )
                            R1= ( -377894195.63531864     , 5.07102403527225857E-003)
                        stable= T
                
                
   iter=            2
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -63797.267330532894     ,  72024.373127371844     )
  coeff of 1/eps   pole amp(1)= ( 1.78472504330784432E-007, 1.03313419193830620E-006)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -3360625.9998586932     ,  72024.383368513212     )
                            R1= (  3296828.7325281603     ,-1.02411413715296131E-002)
                        stable= T
                
                
   iter=            3
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -10346822.767967053     ,  16882400.428735916     )
  coeff of 1/eps   pole amp(1)= ( 1.14844879135489464E-005, 1.53785700553139993E-005)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -58476273.675687447     ,  16882400.942168016     )
                            R1= (  48129450.907720394     ,-0.51343210137290307     )
                        stable= T
                
                
   iter=            4
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -107788.54115603741     ,  82593.162090742990     )
  coeff of 1/eps   pole amp(1)= (-3.31545493281737436E-007,-5.74360391982138995E-007)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -110100.12516387260     ,  82593.161225902077     )
                            R1= (  2311.5840078351903     , 8.64840916222184785E-004)
                        stable= T
                
                
   iter=            5
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  1746787.3491039553     , -213717.61828033614     )
  coeff of 1/eps   pole amp(1)= (-2.73849181553487142E-007,-7.50177417389876519E-008)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  1499191.4219587103     , -213717.61871116390     )
                            R1= (  247595.92714524505     , 4.30827746285127066E-004)
                        stable= T
                
                
   iter=            6
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -370319.46383258700     ,  410967.74881594942     )
  coeff of 1/eps   pole amp(1)= (-2.23808456212282181E-007, 3.00293339096918555E-007)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -50668434.558390886     ,  410967.74885049212     )
                            R1= (  50298115.094558299     ,-3.45426951028434236E-005)
                        stable= T
                
                
   iter=            7
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -106205.49520451674     ,  53749.144159631018     )
  coeff of 1/eps   pole amp(1)= ( 1.75946843228302896E-006, 2.07983113305033296E-006)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -595338.34606520692     ,  53749.144011794109     )
                            R1= (  489132.85086069017     , 1.47836908745816023E-004)
                        stable= T
                
                
   iter=            8
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -89786.646990656503     ,  71990.294360415865     )
  coeff of 1/eps   pole amp(1)= (-4.80277321912581101E-007, 4.57104165709099301E-007)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  274767.10738525318     ,  71990.294532927961     )
                            R1= ( -364553.75437590969     ,-1.72512092435884323E-004)
                        stable= T
                
                
   iter=            9
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  157694.15979564434     ,  1149733.9248735292     )
  coeff of 1/eps   pole amp(1)= (-8.14672489468648564E-007, 5.63326800066400489E-007)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  1204418.9638915253     ,  1149733.9237926416     )
                            R1= ( -1046724.8040958809     , 1.08088755855256834E-003)
                        stable= T
                
                
   iter=           10
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  351241.21367723553     , -203084.81247688702     )
  coeff of 1/eps   pole amp(1)= (-2.07678021979518235E-006,-2.96954463950521433E-007)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  91271.025886653573     , -203084.81041882327     )
                            R1= (  259970.18779058193     ,-2.05806375047176996E-003)
                        stable= T
                
 n_tot =   10.000000000000000     
 n_mp  =   0.0000000000000000     
 n_disc=           0
