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)= ( 2.89250252233020505E-002, 1.1691425591409415 ) coeff of 1/eps pole amp(1)= (-2.59732912396637775E-015,-4.60102327661567013E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 2.89250252233020505E-002, 1.1691425591409415 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -3.5949412619618291 , -2.9724114631840881 ) coeff of 1/eps pole amp(1)= ( 1.38275892472283779E-014, 3.12560161775545214E-016) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.5949412619618291 , -2.9724114631840881 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= (-1.77284703079574682E-002, 5.6136942581183957 ) coeff of 1/eps pole amp(1)= (-3.48911065241753332E-014,-7.44799103741505543E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-1.77284703079574682E-002, 5.6136942581183957 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 6.3157003912640102 , 13.862881328909548 ) coeff of 1/eps pole amp(1)= ( 3.32338323527636703E-014,-3.22874774770758444E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 6.3157003912640102 , 13.862881328909548 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= (-0.20664673099713712 , 3.16225191463089742E-004) coeff of 1/eps pole amp(1)= (-4.21148000100037695E-015, 2.24292089328652257E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.20664673099713712 , 3.16225191463089742E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= (-4.66010522370460742E-002, 5.5057874613103959 ) coeff of 1/eps pole amp(1)= ( 3.02324185380131033E-015, 1.06820339578488061E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-4.66010522370460742E-002, 5.5057874613103959 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= (-0.52679763055963291 , -1.2497687495812182 ) coeff of 1/eps pole amp(1)= ( 1.00289615750492195E-014,-5.33877576633671881E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.52679763055963291 , -1.2497687495812182 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= (-0.12795880437195173 , 0.71164499049295649 ) coeff of 1/eps pole amp(1)= ( 1.58900670399475530E-015, 5.59037062408706315E-015) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-0.12795880437195173 , 0.71164499049295649 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 0.27699069451267572 , 0.55588534440099568 ) coeff of 1/eps pole amp(1)= ( 3.11166023503339773E-016, 6.50244252087914953E-016) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 0.27699069451267572 , 0.55588534440099568 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -3.8486792280099644 , -6.1232999836581543 ) coeff of 1/eps pole amp(1)= (-3.19073211591230227E-014,-1.99611161163333512E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -3.8486792280099644 , -6.1232999836581543 ) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0