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)= ( 53383957.827891409 , 126986265.19427444 ) coeff of 1/eps pole amp(1)= (-1.91573053598403931E-006,-2.55890769902303744E-006) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 431270985.95196068 , 126986265.19818100 ) R1= ( -377887028.12406927 ,-3.90656115193341834E-003) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -63797.261651414679 , 72024.388029756708 ) coeff of 1/eps pole amp(1)= (-7.21112201063078828E-006, 3.74803846968958810E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -363690.85492558568 , 72024.383959787738 ) R1= ( 299893.59327417100 , 4.06996897083351881E-003) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -10346823.490403138 , 16882400.271639138 ) coeff of 1/eps pole amp(1)= ( 2.82423570752143860E-007, 8.63918025621668137E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -58038835.597801164 , 16882400.942260668 ) R1= ( 47692012.107398026 ,-0.67062153050418027 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( -107788.54158113794 , 82593.161228661149 ) coeff of 1/eps pole amp(1)= (-3.03117303701583296E-007,-5.57966151707008687E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -110100.12516228217 , 82593.161225522694 ) R1= ( 2311.5835811442439 , 3.13845385864192118E-006) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 1746787.3486152007 , -213717.61858538873 ) coeff of 1/eps pole amp(1)= (-4.16697730543091893E-007,-3.04460690132950479E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1654732.5929668734 , -213717.61870980682 ) R1= ( 92054.755648327395 , 1.24418084588197097E-004) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -370319.46365982294 , 410967.74880410993 ) coeff of 1/eps pole amp(1)= (-2.38884240388870239E-007, 7.83539033773398308E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -50522553.691372007 , 410967.74885129946 ) R1= ( 50152234.227712184 ,-4.71895196010422717E-005) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -106205.49586043239 , 53749.143876106180 ) coeff of 1/eps pole amp(1)= ( 2.36874257097952068E-006, 1.54470357611323630E-006) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -595338.34610812226 , 53749.144023184585 ) R1= ( 489132.85024768987 ,-1.47078408106866664E-004) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( -89786.648420494806 , 71990.293555912605 ) coeff of 1/eps pole amp(1)= ( 6.40219695924315602E-007, 4.86508675730719698E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -87649.398603700683 , 71990.294534614732 ) R1= ( -2137.2498167941203 ,-9.78702124754581796E-004) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 157694.16187578673 , 1149733.9242085961 ) coeff of 1/eps pole amp(1)= (-4.23553956352407113E-007, 1.99270739272824391E-006) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1204418.9638916375 , 1149733.9237880385 ) R1= ( -1046724.8020158508 , 4.20557470639502636E-004) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( 351241.21235060482 , -203084.80701994590 ) coeff of 1/eps pole amp(1)= (-3.66126187145709991E-008, 3.05851226309012763E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 124119.45354484973 , -203084.81042564716 ) R1= ( 227121.75880575512 , 3.40570124385333826E-003) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000