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)= ( 77834.779048816359 , 210665.04498575244 ) coeff of 1/eps pole amp(1)= ( 5.83099790674168617E-009,-6.22928214780853270E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 84024.357080674527 , 210665.04498574827 ) R1= ( -6189.5780318581683 , 4.17238545935560929E-009) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( 2.9365799109467901 , -45.243909018778851 ) coeff of 1/eps pole amp(1)= (-1.79012360490560241E-011,-3.51530076440109916E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 156.38227565109582 , -45.243909019350056 ) R1= ( -153.44569574014903 , 5.71203165322661741E-010) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -23391.672907094617 , 37974.591875742801 ) coeff of 1/eps pole amp(1)= ( 3.81305653718300164E-010,-6.53989616644570647E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -29361.736096914286 , 37974.591875737868 ) R1= ( 5970.0631898196707 , 4.93673109336345479E-009) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 11.220394483630528 , 13.650693526982979 ) coeff of 1/eps pole amp(1)= ( 1.37070799155480927E-010,-3.00564810754835259E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -35.361989118259565 , 13.650693522703575 ) R1= ( 46.582383601890093 , 4.27940287650585626E-009) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 4722.7174106751372 , 307.17654231476774 ) coeff of 1/eps pole amp(1)= ( 1.63741020742236287E-010, 1.33174153172341559E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 4665.1112448675185 , 307.17654232107964 ) R1= ( 57.606165807619149 ,-6.31187668381771855E-009) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -720.46341258887469 , 1043.5514515318387 ) coeff of 1/eps pole amp(1)= ( 3.69198005500948057E-011,-9.38891098553196630E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2458.1652455152571 , 1043.5514515308173 ) R1= ( 1737.7018329263824 , 1.02144462887920903E-009) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -90.265229657646429 , -89.382756354129640 ) coeff of 1/eps pole amp(1)= (-1.12495790460798162E-010,-1.64473056988045097E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -105.56795310546292 , -89.382756358427642 ) R1= ( 15.302723447816486 , 4.29800568468863292E-009) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 11.149727599402596 , 53.536637176302285 ) coeff of 1/eps pole amp(1)= ( 1.58373980596593356E-010, 1.38409198790095190E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 120.87961240807600 , 53.536637174975844 ) R1= ( -109.72988480867340 , 1.32643940276011563E-009) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -57.396503213027160 , 4715.9796061329462 ) coeff of 1/eps pole amp(1)= ( 5.08812103561240292E-010,-6.66251434923379120E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 179.15280531151009 , 4715.9796061344177 ) R1= ( -236.54930852453725 ,-1.47140384737509648E-009) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -2271.8198270573812 , 834.53073342963512 ) coeff of 1/eps pole amp(1)= ( 8.77889760886318982E-010,-2.54258842414169798E-010) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -2122.3230991902647 , 834.53073343263588 ) R1= ( -149.49672786711656 ,-3.00077633852424597E-009) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000