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)= (-0.10728550383441174 , 0.81607473181265577 ) coeff of 1/eps pole amp(1)= (-3.19923666551591435E-015,-2.88775484163407483E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.10728550383441174 , 0.81607473181265577 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= (-0.75132113659523325 , 1.4786201367289753 ) coeff of 1/eps pole amp(1)= (-2.01227923213309623E-016,-3.82721726719834353E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.75132113659523325 , 1.4786201367289753 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -2.9973507366309620 , 3.3594740661757210 ) coeff of 1/eps pole amp(1)= ( 2.84494650060196363E-016, 1.58810353810217447E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2.9973507366309620 , 3.3594740661757210 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= (-0.79761114554397150 , 1.5336728725090658 ) coeff of 1/eps pole amp(1)= (-1.62630325872825665E-016,-2.07864391048434036E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.79761114554397150 , 1.5336728725090658 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= (-2.97386818392772721E-002, 0.61951380329615702 ) coeff of 1/eps pole amp(1)= (-4.68548810861335596E-015,-4.64663648485168306E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-2.97386818392772721E-002, 0.61951380329615702 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -3.1577828758876514 , 4.1733977270314684 ) coeff of 1/eps pole amp(1)= (-1.19348975147204328E-015, 8.33391462518813891E-016) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.1577828758876514 , 4.1733977270314684 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -1.2335837504776548 , 2.4560711026215865 ) coeff of 1/eps pole amp(1)= ( 5.55111512312578270E-016, 1.02072387081891655E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1.2335837504776548 , 2.4560711026215865 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( -2.4689860892479132 , 4.2884556185442895 ) coeff of 1/eps pole amp(1)= ( 1.00700697780453652E-015,-4.36996279031626282E-016) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2.4689860892479132 , 4.2884556185442895 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -1.4676330447956172 , 3.0394625771986683 ) coeff of 1/eps pole amp(1)= (-3.33066907387546962E-016, 2.71109354340012204E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1.4676330447956172 , 3.0394625771986683 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= (-0.45668416421779795 , 1.5057231563028788 ) coeff of 1/eps pole amp(1)= (-1.90125692967058058E-015,-5.91596523226000819E-017) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.45668416421779795 , 1.5057231563028788 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0