 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 1.8.2                  |
|              Authors: G. Ossola, C. Papadopoulos, R. Pittau          |
|              Published in JHEP 0803:042,2008                         |
|              http://www.ugr.es/~pittau/CutTools                      |
|                                                                      |
|              Compiler with  34  significant digits detetected        |
 ---------------------------------------------------------------------- 
   
########################################################################
#                                                                      #
#                      You are using OneLOop-3.2                       #
#                                                                      #
# for the evaluation of 1-loop scalar 1-, 2-, 3- and 4-point functions #
#                                                                      #
# author: Andreas van Hameren <hamerenREMOVETHIS@ifj.edu.pl>           #
#   date: 19-07-2012                                                   #
#                                                                      #
# 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. #
#                                                                      #
########################################################################
                
   iter=            1
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -63.415977119224912     , -90.510086314917231     )
  coeff of 1/eps   pole amp(1)= (-7.63389351732257637E-013,-1.06391204016131696E-011)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( 1.76373867654469885E-002, -90.510086314890373     )
                            R1= ( -63.433614505990363     ,-2.68528310698457082E-011)
                        stable= T
                
                
   iter=            2
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -195.72595078991671     ,  752.14672612249922     )
  coeff of 1/eps   pole amp(1)= ( 4.83488249436447859E-012, 3.25177186054462566E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -211.26496116304713     ,  752.14672612246488     )
                            R1= (  15.539010373130424     , 3.42936345987254792E-011)
                        stable= T
                
                
   iter=            3
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -506.59199964841702     ,  734.88569401993800     )
  coeff of 1/eps   pole amp(1)= (-1.89708249109798999E-011,-1.65968265998106109E-011)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -507.66606632188956     ,  734.88569401998586     )
                            R1= (  1.0740666734725668     ,-4.78207029530608426E-011)
                        stable= T
                
                
   iter=            4
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -144.22985296229402     ,  437.17321758321128     )
  coeff of 1/eps   pole amp(1)= (-1.64646074551910715E-013, 2.29434141378827292E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -143.47193614008668     ,  437.17321758321435     )
                            R1= (-0.75791682220732959     ,-3.07256442511061291E-012)
                        stable= T
                
                
   iter=            5
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -39.238319415480284     ,  60.450938537130725     )
  coeff of 1/eps   pole amp(1)= (-2.25787444296798867E-012, 9.57717119029936009E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -21.862151299856954     ,  60.450938537350098     )
                            R1= ( -17.376168115623329     ,-2.19370122067630281E-010)
                        stable= T
                
                
   iter=            6
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -1108.8363932732148     ,  2188.4080503268756     )
  coeff of 1/eps   pole amp(1)= ( 9.04701313864109125E-012,-1.26084349565106351E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -1054.0922916036679     ,  2188.4080503268488     )
                            R1= ( -54.744101669546708     , 2.69004374331416336E-011)
                        stable= T
                
                
   iter=            7
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -95.383832305320595     , -135.63530587018403     )
  coeff of 1/eps   pole amp(1)= ( 2.83328915884339949E-012, 4.14924503931957831E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -59.868859758054931     , -135.63530587020841     )
                            R1= ( -35.514972547265671     , 2.43788988996129780E-011)
                        stable= T
                
                
   iter=            8
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  275.87708782965763     , -1075.4435023405863     )
  coeff of 1/eps   pole amp(1)= (-1.30562227695918409E-013,-1.26446956456907529E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  276.91492722481286     , -1075.4435023406136     )
                            R1= ( -1.0378393951552312     , 2.72284417235368924E-011)
                        stable= T
                
                
   iter=            9
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (  169.04049810059541     , -950.12871340833601     )
  coeff of 1/eps   pole amp(1)= (-1.20338461417901499E-012, 2.08091179772823377E-012)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (  169.62153632401416     , -950.12871340833703     )
                            R1= (-0.58103822341873013     , 1.05018216345342735E-012)
                        stable= T
                
                
   iter=           10
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( -66.441853461941434     , -211.72014200395145     )
  coeff of 1/eps   pole amp(1)= ( 5.98965321785271954E-014,-1.21584543317031908E-013)
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( -54.986674200891962     , -211.72014200389395     )
                            R1= ( -11.455179261049473     ,-5.74889469362460685E-011)
                        stable= T
                
 n_tot =   10.000000000000000     
 n_mp  =   0.0000000000000000     
 n_unst=   0.0000000000000000     
