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)= ( 172.54098281106576 , 9.2741742880435272 ) coeff of 1/eps pole amp(1)= (-2.74948674938713111E-011,-2.18906388844759318E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 59.401534030701036 , 9.2741742869904780 ) R1= ( 113.13944878036473 , 1.05304913677883864E-009) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( 1018.3486368279524 , 4.7046981756768425 ) coeff of 1/eps pole amp(1)= ( 5.12523357087957265E-012, 7.69428588268720710E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1047.8902744464838 , 4.7046981759146735 ) R1= ( -29.541637618531329 ,-2.37830999338939385E-010) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( 532.51454673432261 , 1136.6339828661160 ) coeff of 1/eps pole amp(1)= ( 2.34915975561023060E-011,-4.70284357694799563E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 575.52031805391800 , 1136.6339828660416 ) R1= ( -43.005771319595411 , 7.43584860352086656E-011) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 3783.4094968246723 , 4818.9436112226040 ) coeff of 1/eps pole amp(1)= ( 1.77913239696181336E-011, 5.47002691422312597E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 3709.7235662251519 , 4818.9436112226249 ) R1= ( 73.685930599520219 ,-2.06923755907695301E-011) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 72.659407400837893 , -253.35892493840620 ) coeff of 1/eps pole amp(1)= (-1.41640033035628221E-010, 1.02858350501735924E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 70.058538083497226 , -253.35892493807157 ) R1= ( 2.6008693173406670 ,-3.34645378075038138E-010) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( 601.51490618522269 , 2432.1786077691286 ) coeff of 1/eps pole amp(1)= ( 2.02975414254069619E-011, 2.06158614148091423E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 634.96470285298460 , 2432.1786077680067 ) R1= ( -33.449796667761923 , 1.12189617595959139E-009) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( 319.19223871423276 , 128.57104985994840 ) coeff of 1/eps pole amp(1)= ( 2.82340817392423560E-012,-2.38166706746161774E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 266.26179844791778 , 128.57104986028500 ) R1= ( 52.930440266314989 ,-3.36596528427435260E-010) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 370.44079924206721 , 219.70141803227762 ) coeff of 1/eps pole amp(1)= (-3.61808361049043015E-011, 8.15758623175957862E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1630.4767096960468 , 219.70141803232397 ) R1= ( 2000.9175089381140 ,-4.63665550398672999E-011) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 186.45174651631010 , -125.50808863637738 ) coeff of 1/eps pole amp(1)= (-6.37601083042227401E-012, 7.05819706388615061E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 172.40937827028236 , -125.50808863662120 ) R1= ( 14.042368246027728 , 2.43822029233342629E-010) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( 2034.5062065811924 , 2080.5011907858616 ) coeff of 1/eps pole amp(1)= (-2.64767319180236882E-010,-2.96424109980023553E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1968.9813479036379 , 2080.5011907866920 ) R1= ( 65.524858677554462 ,-8.30523028128027404E-010) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0