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)= ( -63.415977119186991 , -90.510086314917629 ) coeff of 1/eps pole amp(1)= (-1.10509518203016910E-012,-1.05193362661739200E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1.76373868033740666E-002, -90.510086314890771 ) R1= ( -63.433614505990363 ,-2.68528310698457082E-011) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= ( -195.72595079235998 , 752.14672612318248 ) coeff of 1/eps pole amp(1)= ( 1.96144489539307187E-012,-8.68837353593610488E-014) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -211.26496116549038 , 752.14672612320669 ) R1= ( 15.539010373130395 ,-2.42494024860207037E-011) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= ( -506.59199964851149 , 734.88569401998018 ) coeff of 1/eps pole amp(1)= (-1.77735604012241311E-011,-1.86395804840031573E-011) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -507.66606632190900 , 734.88569401997472 ) R1= ( 1.0740666733974873 , 5.42785816293189815E-012) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( -144.22985296229839 , 437.17321758321759 ) coeff of 1/eps pole amp(1)= (-1.64646074551910715E-013, 2.29434141378827292E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -143.47193614009106 , 437.17321758322066 ) R1= (-0.75791682220732959 ,-3.07256442511061291E-012) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= ( -39.238319415699124 , 60.450938539651439 ) coeff of 1/eps pole amp(1)= (-6.16169268385924340E-012, 5.26354926299332812E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -21.862151299703303 , 60.450938539580306 ) R1= ( -17.376168115995824 , 7.11310121914721042E-011) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= ( -1108.8363932732616 , 2188.4080503268929 ) coeff of 1/eps pole amp(1)= ( 8.14340261889867634E-012,-9.34675788032950089E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -1054.0922916036686 , 2188.4080503268488 ) R1= ( -54.744101669593050 , 4.39989378264726786E-011) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( -95.383832305321761 , -135.63530587018286 ) coeff of 1/eps pole amp(1)= ( 2.83328915884339949E-012, 4.14924503931957831E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -59.868859758056082 , -135.63530587020725 ) R1= ( -35.514972547265671 , 2.43788988996129780E-011) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= ( 275.87708782965990 , -1075.4435023405886 ) coeff of 1/eps pole amp(1)= (-1.12798659301915905E-013,-1.25609579606279140E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 276.91492722481468 , -1075.4435023406149 ) R1= ( -1.0378393951547658 , 2.63189470217639642E-011) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= ( 169.04049810059553 , -950.12871340833249 ) coeff of 1/eps pole amp(1)= (-1.17936216348368816E-012, 2.24317974671050667E-012) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 169.62153632401424 , -950.12871340833351 ) R1= (-0.58103822341873013 , 1.05018216345342735E-012) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= ( -66.441853461965962 , -211.72014200390259 ) coeff of 1/eps pole amp(1)= ( 5.98965321785271954E-014,-1.21584543317031908E-013) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( -54.986674200916497 , -211.72014200384510 ) R1= ( -11.455179261049473 ,-5.74889469362460685E-011) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0