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)= ( 77834.779048846380 , 210665.04498575686 ) coeff of 1/eps pole amp(1)= ( 1.00698684946110006E-008,-9.63190028785021844E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 84024.357080695365 , 210665.04498577159 ) R1= ( -6189.5780318489878 ,-1.47151645535359441E-008) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( 2.9365797108784761 , -45.243908938505136 ) coeff of 1/eps pole amp(1)= ( 2.90873325425877738E-010, 1.68615741497265182E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 156.38227548424499 , -45.243908950897072 ) R1= ( -153.44569577336651 , 1.23919332795097151E-008) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -23391.672907069951 , 37974.591875738479 ) coeff of 1/eps pole amp(1)= ( 3.02406988339498639E-010,-4.73282950660557437E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -29361.736096918463 , 37974.591875733044 ) R1= ( 5970.0631898485099 , 5.43580827641609882E-009) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 11.220394488085688 , 13.650693522230842 ) coeff of 1/eps pole amp(1)= (-4.14643250290502863E-011,-6.45303903123147950E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -35.361989112683091 , 13.650693522177285 ) R1= ( 46.582383600768779 , 5.35576916149695060E-011) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 4722.7174106680477 , 307.17654231945698 ) coeff of 1/eps pole amp(1)= ( 2.38209452163573587E-011,-3.77664923680101279E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 4665.1112448673684 , 307.17654232023921 ) R1= ( 57.606165800679520 ,-7.82225281770187978E-010) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -720.46341258793859 , 1043.5514515303948 ) coeff of 1/eps pole amp(1)= (-4.83737494505476207E-011,-3.88885252841867230E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2458.1652455151611 , 1043.5514515301832 ) R1= ( 1737.7018329272225 , 2.11706996378069345E-010) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -90.265229666506741 , -89.382756371052409 ) coeff of 1/eps pole amp(1)= (-8.91011708858968632E-011, 1.53835430595252475E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -105.56795311808551 , -89.382756373240284 ) R1= ( 15.302723451578764 , 2.18787903349948448E-009) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 11.149727586575281 , 53.536637181298133 ) coeff of 1/eps pole amp(1)= ( 1.07517439396076497E-010, 1.52877427812376368E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 120.87961239913756 , 53.536637178303451 ) R1= ( -109.72988481256228 , 2.99468503328625965E-009) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -57.396503211365655 , 4715.9796061225652 ) coeff of 1/eps pole amp(1)= ( 2.92300239568277220E-010,-1.01753920750402322E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 179.15280531062632 , 4715.9796061304451 ) R1= ( -236.54930852199197 ,-7.87985260861101577E-009) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -2271.8198274458960 , 834.53073338254819 ) coeff of 1/eps pole amp(1)= ( 4.19716172928019660E-009, 2.98086882723809297E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2122.3230995799731 , 834.53073338215177 ) R1= ( -149.49672786592291 , 3.96480892561612605E-010) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0