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)= ( 110.91756908632418 , 350.13765392138680 ) coeff of 1/eps pole amp(1)= (-6.60721477530046286E-013, 1.22250875252493559E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 110.91756908632418 , 350.13765392138680 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= (-0.10524868431067459 ,-0.21586714698518003 ) coeff of 1/eps pole amp(1)= (-1.06245793209829888E-012, 1.98526096691146393E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.10524868431067459 ,-0.21586714698518003 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -53.688937899117562 , 87.262758819741066 ) coeff of 1/eps pole amp(1)= ( 5.96861362417433483E-012, 3.69895775192085084E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -53.688937899117562 , 87.262758819741066 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 0.14787511650627991 , 0.61788313538053574 ) coeff of 1/eps pole amp(1)= (-6.30467900109010770E-014,-3.55597554840692998E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 0.14787511650627991 , 0.61788313538053574 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 11.783249527971504 , 3.6780170639586665 ) coeff of 1/eps pole amp(1)= (-9.04662866699820073E-015,-2.92404170835385665E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 11.783249527971504 , 3.6780170639586665 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -1.9837637545410298 , 3.3100567640772320 ) coeff of 1/eps pole amp(1)= (-5.96619313689503031E-014,-1.69495041979508650E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1.9837637545410298 , 3.3100567640772320 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= (-0.25548083120625370 , 7.23890727928302447E-002) coeff of 1/eps pole amp(1)= ( 2.74231863345991700E-014,-3.86345040685562017E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.25548083120625370 , 7.23890727928302447E-002) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= (-6.77668364252278273E-003,-0.22941256486116193 ) coeff of 1/eps pole amp(1)= (-8.04554271948672371E-014,-3.15702896073849905E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-6.77668364252278273E-003,-0.22941256486116193 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -3.6144152703332901 , 19.606148550976368 ) coeff of 1/eps pole amp(1)= ( 2.97372543256457789E-012, 3.78576715198154337E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.6144152703332901 , 19.606148550976368 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( 10.266962124962715 ,-0.47903402142238710 ) coeff of 1/eps pole amp(1)= ( 5.29330287858347214E-013,-5.39504581255403021E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 10.266962124962715 ,-0.47903402142238710 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000