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)= ( 65088.321964060131 , 3057.9616206004675 ) coeff of 1/eps pole amp(1)= (-6.88478742461029469E-007, 4.91614696582851558E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -211993.50444436760 , 3057.9615515528189 ) R1= ( 277081.82640842773 , 6.90476483697120369E-005) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -196960.33084427047 , 86259.175803803519 ) coeff of 1/eps pole amp(1)= (-1.82345729626831599E-008, 2.63030763917048014E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -80353.840975688945 , 86259.175805420353 ) R1= ( -116606.48986858154 ,-1.61684100236746830E-006) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( 324920.73699045269 , 152372.82334079975 ) coeff of 1/eps pole amp(1)= (-1.14767999548348598E-008, 1.84733815294199025E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 544115.86823907006 , 152372.82335284670 ) R1= ( -219195.13124861737 ,-1.20469409685058754E-005) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 2088806.0847748485 , 1715981.6164475651 ) coeff of 1/eps pole amp(1)= (-6.13019892625743523E-008, 3.66684620084537040E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 2211168.8463380053 , 1715981.6164733369 ) R1= ( -122362.76156315667 ,-2.57718130217975408E-005) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( 14070.390284990819 , 23784.948299247590 ) coeff of 1/eps pole amp(1)= ( 1.56857572619628627E-006,-8.13194014431254113E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -26786.645873115922 , 23784.948602995701 ) R1= ( 40857.036158106741 ,-3.03748109378162566E-004) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( 594279.86569779832 , 1169582.1065074331 ) coeff of 1/eps pole amp(1)= (-2.91799437945883255E-007,-3.10530550493663718E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 702778.07913202082 , 1169582.1071973043 ) R1= ( -108498.21343422256 ,-6.89871122627706921E-004) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -118338.91523682680 , 32190.115934844878 ) coeff of 1/eps pole amp(1)= ( 2.53982079811976291E-008, 5.33062440019451907E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -114616.52933924810 , 32190.115958792874 ) R1= ( -3722.3858975786989 ,-2.39479953777522336E-005) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 100943.72065144591 , 51876.552633169355 ) coeff of 1/eps pole amp(1)= (-3.81260178983211517E-008, 6.46786931994222651E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -13651364.156665539 , 51876.552642101735 ) R1= ( 13752307.877316985 ,-8.93237780275585659E-006) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 86174.766069342964 , -92297.029398674465 ) coeff of 1/eps pole amp(1)= ( 2.66311417362885550E-009, 1.83717582586651906E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 102768.33394068088 , -92297.029398284722 ) R1= ( -16593.567871337909 ,-3.89743204788881671E-007) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -993202.95313087956 , -661314.62382726104 ) coeff of 1/eps pole amp(1)= ( 2.86134877569566015E-007,-1.26400259218388632E-007) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -905453.76897572854 , -661314.62456633453 ) R1= ( -87749.184155151015 , 7.39073551475977653E-004) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_unst= 0.0000000000000000