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 1.6.9 | | 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 # # 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)= ( 110.91756908639330 , 350.13765392137543 ) coeff of 1/eps pole amp(1)= (-1.00633390509585752E-012, 4.09334150258064000E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 110.91756908639330 , 350.13765392137543 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= (-0.10524868451556642 ,-0.21586714695200157 ) coeff of 1/eps pole amp(1)= ( 1.06714506345082991E-013,-1.77334451505451228E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.10524868451556642 ,-0.21586714695200157 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -53.688937899118706 , 87.262758819746693 ) coeff of 1/eps pole amp(1)= ( 5.53972796454860195E-012, 2.93969026754519238E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -53.688937899118706 , 87.262758819746693 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 0.14787511650645022 , 0.61788313537493766 ) coeff of 1/eps pole amp(1)= (-1.17295062551647788E-013,-7.01770601700114492E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 0.14787511650645022 , 0.61788313537493766 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 11.783249527972552 , 3.6780170639568861 ) coeff of 1/eps pole amp(1)= (-2.10534740919946558E-013, 2.10004137936725657E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 11.783249527972552 , 3.6780170639568861 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -1.9837637545388647 , 3.3100567640787504 ) coeff of 1/eps pole amp(1)= (-3.09063281575956391E-013,-1.30628229143400225E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1.9837637545388647 , 3.3100567640787504 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= (-0.25548083121659759 , 7.23890727786941773E-002) coeff of 1/eps pole amp(1)= (-1.53653673985731931E-014,-1.00621742126705482E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.25548083121659759 , 7.23890727786941773E-002) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= (-6.77668363559281485E-003,-0.22941256486366604 ) coeff of 1/eps pole amp(1)= (-1.67487484372320537E-014,-9.02374284930266792E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-6.77668363559281485E-003,-0.22941256486366604 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -3.6144152704245216 , 19.606148550995130 ) coeff of 1/eps pole amp(1)= ( 3.18182025865754170E-012, 3.83594237437696151E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.6144152704245216 , 19.606148550995130 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( 10.266962124956558 ,-0.47903402143260038 ) coeff of 1/eps pole amp(1)= (-2.12083288354061883E-014, 2.10565479032032037E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 10.266962124956558 ,-0.47903402143260038 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0