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 1.9.3 | | 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-3.4 # # # # for the evaluation of 1-loop scalar 1-, 2-, 3- and 4-point functions # # # # author: Andreas van Hameren # # date: 02-01-2014 # # # # 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)= ( 172.54098280591393 , 9.2741742833764338 ) coeff of 1/eps pole amp(1)= (-1.29930094461272461E-010,-5.82353331977294973E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 59.401534026955090 , 9.2741742851590576 ) R1= ( 113.13944877895882 ,-1.78262353767166819E-009) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( 1018.3486368270835 , 4.7046981766469802 ) coeff of 1/eps pole amp(1)= ( 8.06910094297563774E-013, 8.36390472279856567E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1047.8902744465818 , 4.7046981758669064 ) R1= ( -29.541637619498285 , 7.80073872164166439E-010) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( 532.51454673510932 , 1136.6339828643675 ) coeff of 1/eps pole amp(1)= ( 4.28240776173538507E-012,-5.33660612209096735E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 575.52031805415788 , 1136.6339828658611 ) R1= ( -43.005771319048520 ,-1.49365670942813738E-009) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 3783.4094967596238 , 4818.9436112145468 ) coeff of 1/eps pole amp(1)= (-2.54419041390008260E-010,-8.66468373609023221E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 3709.7235661637696 , 4818.9436112142521 ) R1= ( 73.685930595854174 , 2.94603802464266189E-010) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 72.659407398559892 , -253.35892493966261 ) coeff of 1/eps pole amp(1)= (-5.86235504584919909E-011, 2.22637600221522151E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 70.058538081343798 , -253.35892493821697 ) R1= ( 2.6008693172160910 ,-1.44565071025226644E-009) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( 601.51490618503192 , 2432.1786077691268 ) coeff of 1/eps pole amp(1)= ( 1.36258226923757775E-011, 4.72451021139658928E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 634.96470285324131 , 2432.1786077680590 ) R1= ( -33.449796668209430 , 1.06788835552151808E-009) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( 319.19223871123148 , 128.57104986086225 ) coeff of 1/eps pole amp(1)= ( 1.34649513761075923E-011,-9.45319048482053492E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 266.26179844686311 , 128.57104986056217 ) R1= ( 52.930440264368386 , 3.00088487392713412E-010) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 370.44079931090982 , 219.70141804227779 ) coeff of 1/eps pole amp(1)= ( 6.80699940858175978E-012, 3.42940421858615535E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1630.4767096287308 , 219.70141804083792 ) R1= ( 2000.9175089396406 , 1.43988101442005237E-009) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 186.45174650846457 , -125.50808863690608 ) coeff of 1/eps pole amp(1)= (-1.61635149709127290E-011, 7.77240192909552690E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 172.40937826199229 , -125.50808863702450 ) R1= ( 14.042368246472293 , 1.18415144356731544E-010) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( 2034.5062053944896 , 2080.5011907844291 ) coeff of 1/eps pole amp(1)= ( 1.28071945409979904E-011, 4.18861682916749119E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1968.9813467150259 , 2080.5011907859121 ) R1= ( 65.524858679463790 ,-1.48270373756531626E-009) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000