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)= ( 0.15274950114173860 , 0.58345126755575594 ) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 0.15274950114173860 , 0.58345126755575594 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( 9.26989688931154228E-005, 1.08070427873700718E-004) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 9.26989688931154228E-005, 1.08070427873700718E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= (-0.12273998344219260 , 0.20528981832389467 ) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.12273998344219260 , 0.20528981832389467 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= (-1.02531658684248636E-003,-5.86030787701769841E-003) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-1.02531658684248636E-003,-5.86030787701769841E-003) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 2.86315119312698582E-002, 1.72558090280294611E-002) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 2.86315119312698582E-002, 1.72558090280294611E-002) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= (-5.59989194644450530E-003, 9.90645494412226851E-003) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-5.59989194644450530E-003, 9.90645494412226851E-003) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= (-2.50246154230501121E-004, 1.54227612624131317E-003) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-2.50246154230501121E-004, 1.54227612624131317E-003) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= (-7.24719116218538128E-004,-4.70253747587758041E-004) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-7.24719116218538128E-004,-4.70253747587758041E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= (-2.57702189360526010E-002, 7.90396085760030620E-002) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-2.57702189360526010E-002, 7.90396085760030620E-002) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= (-5.45514105257700818E-002,-1.35105057407527446E-002) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-5.45514105257700818E-002,-1.35105057407527446E-002) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0