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)= (-0.10728550383454354 , 0.81607473181264822 ) coeff of 1/eps pole amp(1)= (-1.70870262383715499E-016,-3.90162437247010935E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.10728550383454354 , 0.81607473181264822 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= (-0.75132113659545507 , 1.4786201367290346 ) coeff of 1/eps pole amp(1)= ( 1.50573997714786856E-015,-6.82469910821949124E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.75132113659545507 , 1.4786201367290346 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -2.9973507366309762 , 3.3594740661757183 ) coeff of 1/eps pole amp(1)= (-1.12757025938492461E-017, 1.75444269771324771E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2.9973507366309762 , 3.3594740661757183 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= (-0.79761114554389279 , 1.5336728725090183 ) coeff of 1/eps pole amp(1)= (-3.51932025188794739E-016,-1.82858090689019125E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.79761114554389279 , 1.5336728725090183 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= (-2.97386818387874174E-002, 0.61951380329603289 ) coeff of 1/eps pole amp(1)= (-4.37323788293753069E-015,-2.96860821123537261E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-2.97386818387874174E-002, 0.61951380329603289 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -3.1577828758875630 , 4.1733977270314879 ) coeff of 1/eps pole amp(1)= ( 3.60822483003175876E-016, 2.89405452819065772E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.1577828758875630 , 4.1733977270314879 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -1.2335837504776375 , 2.4560711026215944 ) coeff of 1/eps pole amp(1)= (-2.22044604925031308E-015, 8.28252625262081010E-017) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1.2335837504776375 , 2.4560711026215944 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( -2.4689860892478919 , 4.2884556185442717 ) coeff of 1/eps pole amp(1)= ( 6.43582409587395432E-016, 3.07710846760681157E-016) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2.4689860892478919 , 4.2884556185442717 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -1.4676330447956174 , 3.0394625771986723 ) coeff of 1/eps pole amp(1)= ( 6.66133814775093924E-016,-8.55177854952909161E-017) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1.4676330447956174 , 3.0394625771986723 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= (-0.45668416421782698 , 1.5057231563028670 ) coeff of 1/eps pole amp(1)= (-9.71445146547011973E-017,-2.30899160210593773E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.45668416421782698 , 1.5057231563028670 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000