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)= ( -507883.66574964579 , 217964.05182264186 ) coeff of 1/eps pole amp(1)= ( 113101.34112262928 ,-2.21455818259138325E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -659883.21308153076 , 217964.05177363113 ) R1= ( 151999.54733188497 , 4.90107434449576007E-005) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -549520.17431077838 , 562915.10215739638 ) coeff of 1/eps pole amp(1)= ( 113101.34112257768 , 3.39236229779166224E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -660104.27128180314 , 562915.10219433799 ) R1= ( 110584.09697102476 ,-3.69415981506577456E-005) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -542184.46424828726 , 471124.65731598414 ) coeff of 1/eps pole amp(1)= ( 113101.34112259586 , 2.89737990330287700E-008) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -748278.28550470027 , 471124.65732085053 ) R1= ( 206093.82125641301 ,-4.86639713854603481E-006) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( -495832.52671583998 , 363827.38932256645 ) coeff of 1/eps pole amp(1)= ( 113101.34112263941 , 5.69812721736364104E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -707361.21828619519 , 363827.38931782270 ) R1= ( 211528.69157035518 , 4.74372145287866232E-006) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( -527397.47946158820 , 188292.69755391558 ) coeff of 1/eps pole amp(1)= ( 113101.34112259414 ,-5.81444441217078087E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -651552.65657378477 , 188292.69767420372 ) R1= ( 124155.17711219660 ,-1.20288147665492055E-004) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -852948.48382930970 , 1416928.7575200545 ) coeff of 1/eps pole amp(1)= ( 113101.34112263580 , 4.19892400346953034E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -948263.85509999481 , 1416928.7575234913 ) R1= ( 95315.371270685107 ,-3.43680266624240389E-006) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -463367.59718789079 , 347931.91080027015 ) coeff of 1/eps pole amp(1)= ( 113101.34112261461 ,-8.87131157708733251E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -564936.25940927293 , 347931.91082471010 ) R1= ( 101568.66222138212 ,-2.44399501690569644E-005) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( -505287.70511045551 , 632970.45778795390 ) coeff of 1/eps pole amp(1)= ( 113101.34112263734 ,-1.44254717533098647E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1005372.4646214396 , 632970.45778795262 ) R1= ( 500084.75951098406 , 1.25435066171453795E-009) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( -486802.18041622831 , 632420.98749838886 ) coeff of 1/eps pole amp(1)= ( 113101.34112264258 , 7.79377117745140395E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -538682.25705550611 , 632420.98749867838 ) R1= ( 51880.076639277810 ,-2.89549301754016396E-007) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -463951.19803286705 , 311217.16144117992 ) coeff of 1/eps pole amp(1)= ( 113101.34112264162 ,-1.71835534591876946E-009) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -561475.15333439654 , 311217.16145058081 ) R1= ( 97523.955301529495 ,-9.40087728253325767E-006) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0