 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)= (-1.10581082351118079E-005, 3.82757143995054834E-005)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-1.10581082351118079E-005, 3.82757143995054834E-005)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            2
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-6.08823179391560724E-005,-1.22143014817594674E-004)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-6.08823179391560724E-005,-1.22143014817594674E-004)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            3
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-4.72115910175283397E-005, 1.14113770754292865E-004)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-4.72115910175283397E-005, 1.14113770754292865E-004)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            4
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( 2.70399434697404534E-005, 1.75049104459220527E-004)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( 2.70399434697404534E-005, 1.75049104459220527E-004)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            5
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-2.07096851426084388E-006,-5.30949884696294093E-006)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-2.07096851426084388E-006,-5.30949884696294093E-006)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            6
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-2.11139839390537274E-005, 5.43370217248214911E-005)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-2.11139839390537274E-005, 5.43370217248214911E-005)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            7
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= ( 1.13085667228763524E-006,-1.29035666519133749E-005)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= ( 1.13085667228763524E-006,-1.29035666519133749E-005)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            8
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-5.99127706399224493E-006, 2.74144985550398823E-006)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-5.99127706399224493E-006, 2.74144985550398823E-006)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=            9
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-6.40182901121604650E-006, 8.91217226231079370E-006)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-6.40182901121604650E-006, 8.91217226231079370E-006)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
                
   iter=           10
                
                
  Complete Amplitude (without r2):     
                
                
  finite part           amp(0)= (-8.88730499584883462E-006,-4.29134704900984671E-005)
  coeff of 1/eps   pole amp(1)= (  0.0000000000000000     ,  0.0000000000000000     )
  coeff of 1/eps^2 pole amp(2)= (  0.0000000000000000     ,  0.0000000000000000     )
                         ampcc= (-8.88730499584883462E-006,-4.29134704900984671E-005)
                            R1= (  0.0000000000000000     ,  0.0000000000000000     )
                        stable= T
                
 n_tot =   10.000000000000000     
 n_mp  =   0.0000000000000000     
 n_disc=           0
