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)= ( 2.89250252248215017E-002, 1.1691425591406408 ) coeff of 1/eps pole amp(1)= ( 1.72326557659600345E-014,-1.01353943545931134E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 2.89250252248215017E-002, 1.1691425591406408 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -3.5949412619622896 , -2.9724114631842120 ) coeff of 1/eps pole amp(1)= ( 1.54127470335108097E-014, 2.75852045530283418E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.5949412619622896 , -2.9724114631842120 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= (-1.77284703077160710E-002, 5.6136942581181808 ) coeff of 1/eps pole amp(1)= (-4.22687397778377660E-014, 1.36151711573628590E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-1.77284703077160710E-002, 5.6136942581181808 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 6.3157003908495506 , 13.862881328865479 ) coeff of 1/eps pole amp(1)= ( 4.93609710397469037E-013,-3.20495497518010316E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 6.3157003908495506 , 13.862881328865479 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= (-0.20664673099703648 , 3.16225191578293813E-004) coeff of 1/eps pole amp(1)= (-1.28717159543836890E-015,-3.51684924836148163E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.20664673099703648 , 3.16225191578293813E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= (-4.66010522369231864E-002, 5.5057874613105389 ) coeff of 1/eps pole amp(1)= ( 4.61826079765567665E-015,-5.46824777314782881E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-4.66010522369231864E-002, 5.5057874613105389 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= (-0.52679763047437023 , -1.2497687495812937 ) coeff of 1/eps pole amp(1)= (-5.42621503285545259E-015, 2.88250267097056881E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.52679763047437023 , -1.2497687495812937 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= (-0.12795880447546176 , 0.71164499047980112 ) coeff of 1/eps pole amp(1)= ( 1.93650027653993750E-015, 3.00704611161950889E-016) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.12795880447546176 , 0.71164499047980112 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 0.27699069449999097 , 0.55588534440196491 ) coeff of 1/eps pole amp(1)= (-9.99959663683380739E-015,-8.31286983157405258E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 0.27699069449999097 , 0.55588534440196491 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -3.8486792280310609 , -6.1232999836583160 ) coeff of 1/eps pole amp(1)= (-1.13385558266673042E-014,-7.74587771950606970E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.8486792280310609 , -6.1232999836583160 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000