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)= ( 53383957.821603358 , 126986265.20322932 ) coeff of 1/eps pole amp(1)= (-1.83719203050713986E-006,-1.19366438964925456E-006) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 431278153.45692199 , 126986265.19815829 ) R1= ( -377894195.63531864 , 5.07102403527225857E-003) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -63797.267330532894 , 72024.373127371844 ) coeff of 1/eps pole amp(1)= ( 1.78472504330784432E-007, 1.03313419193830620E-006) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3360625.9998586932 , 72024.383368513212 ) R1= ( 3296828.7325281603 ,-1.02411413715296131E-002) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -10346822.767967053 , 16882400.428735916 ) coeff of 1/eps pole amp(1)= ( 1.14844879135489464E-005, 1.53785700553139993E-005) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -58476273.675687447 , 16882400.942168016 ) R1= ( 48129450.907720394 ,-0.51343210137290307 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( -107788.54115603741 , 82593.162090742990 ) coeff of 1/eps pole amp(1)= (-3.31545493281737436E-007,-5.74360391982138995E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -110100.12516387260 , 82593.161225902077 ) R1= ( 2311.5840078351903 , 8.64840916222184785E-004) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 1746787.3491039553 , -213717.61828033614 ) coeff of 1/eps pole amp(1)= (-2.73849181553487142E-007,-7.50177417389876519E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1499191.4219587103 , -213717.61871116390 ) R1= ( 247595.92714524505 , 4.30827746285127066E-004) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -370319.46383258700 , 410967.74881594942 ) coeff of 1/eps pole amp(1)= (-2.23808456212282181E-007, 3.00293339096918555E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -50668434.558390886 , 410967.74885049212 ) R1= ( 50298115.094558299 ,-3.45426951028434236E-005) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -106205.49520451674 , 53749.144159631018 ) coeff of 1/eps pole amp(1)= ( 1.75946843228302896E-006, 2.07983113305033296E-006) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -595338.34606520692 , 53749.144011794109 ) R1= ( 489132.85086069017 , 1.47836908745816023E-004) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( -89786.646990656503 , 71990.294360415865 ) coeff of 1/eps pole amp(1)= (-4.80277321912581101E-007, 4.57104165709099301E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 274767.10738525318 , 71990.294532927961 ) R1= ( -364553.75437590969 ,-1.72512092435884323E-004) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 157694.15979564434 , 1149733.9248735292 ) coeff of 1/eps pole amp(1)= (-8.14672489468648564E-007, 5.63326800066400489E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1204418.9638915253 , 1149733.9237926416 ) R1= ( -1046724.8040958809 , 1.08088755855256834E-003) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( 351241.21367723553 , -203084.81247688702 ) coeff of 1/eps pole amp(1)= (-2.07678021979518235E-006,-2.96954463950521433E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 91271.025886653573 , -203084.81041882327 ) R1= ( 259970.18779058193 ,-2.05806375047176996E-003) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0