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)= ( -63.415977119253625 , -90.510086314632588 ) coeff of 1/eps pole amp(1)= ( 1.63043190060108145E-012,-1.64857874178971422E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1.76373867717513483E-002, -90.510086314914403 ) R1= ( -63.433614506025378 , 2.81818302028113986E-010) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -195.72595079226886 , 752.14672612203651 ) coeff of 1/eps pole amp(1)= (-8.04185884550889796E-012,-1.54093698782129478E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -211.26496116493362 , 752.14672612287461 ) R1= ( 15.539010372664762 ,-8.38110736367525574E-010) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -506.59199964805936 , 734.88569402002338 ) coeff of 1/eps pole amp(1)= (-2.05799821628716018E-011,-9.09325421369707763E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -507.66606632188365 , 734.88569401998268 ) R1= ( 1.0740666738242677 , 4.06743971836931476E-011) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( -144.22985296252676 , 437.17321758330650 ) coeff of 1/eps pole amp(1)= ( 5.51225731726390222E-014, 3.04441987490268187E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -143.47193614008734 , 437.17321758321890 ) R1= (-0.75791682243943992 , 8.76164918395261416E-011) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( -39.238319414977795 , 60.450938538083115 ) coeff of 1/eps pole amp(1)= ( 1.24431801667990172E-011,-8.08473868960806191E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -21.862151299727078 , 60.450938537451279 ) R1= ( -17.376168115250721 , 6.31837338005425388E-010) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -1108.8363932732591 , 2188.4080503266405 ) coeff of 1/eps pole amp(1)= ( 9.49748613088274851E-012,-6.26455041425696902E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1054.0922916036677 , 2188.4080503268497 ) R1= ( -54.744101669591331 ,-2.09221440172768775E-010) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -95.383832304777656 , -135.63530586981975 ) coeff of 1/eps pole amp(1)= ( 1.28785870856518159E-012, 7.00903838616795050E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -59.868859758060395 , -135.63530587020887 ) R1= ( -35.514972546717267 , 3.89128063105204092E-010) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 275.87708782987698 , -1075.4435023412107 ) coeff of 1/eps pole amp(1)= (-1.58983937126322417E-013,-9.02963084943513586E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 276.91492722481433 , -1075.4435023406113 ) R1= ( -1.0378393949373539 ,-5.99424776481782870E-010) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 169.04049810038907 , -950.12871340818378 ) coeff of 1/eps pole amp(1)= (-1.18106913138404934E-012, 2.03160958550507606E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 169.62153632401410 , -950.12871340833681 ) R1= (-0.58103822362502200 , 1.53022483573295176E-010) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -66.441853461846023 , -211.72014200367141 ) coeff of 1/eps pole amp(1)= ( 3.78030939884865802E-014,-6.65936496127973901E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -54.986674200889659 , -211.72014200389708 ) R1= ( -11.455179260956371 , 2.25659491093210818E-010) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000