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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 1.9.0 |
| 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-3.2 #
# #
# for the evaluation of 1-loop scalar 1-, 2-, 3- and 4-point functions #
# #
# author: Andreas van Hameren <hamerenREMOVETHIS@ifj.edu.pl> #
# date: 19-07-2012 #
# #
# 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)= ( 2.29684837518455420E-007, 1.67257437866697418E-006)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= ( 2.29684837518455420E-007, 1.67257437866697418E-006)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 2
Complete Amplitude (without r2):
finite part amp(0)= (-3.86240283547311229E-009, 5.33820913782236040E-009)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-3.86240283547311229E-009, 5.33820913782236040E-009)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 3
Complete Amplitude (without r2):
finite part amp(0)= (-4.68320060774638477E-007, 1.68237308380606308E-006)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-4.68320060774638477E-007, 1.68237308380606308E-006)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 4
Complete Amplitude (without r2):
finite part amp(0)= ( 5.01046940724204958E-008,-1.82029130561423645E-007)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= ( 5.01046940724204958E-008,-1.82029130561423645E-007)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 5
Complete Amplitude (without r2):
finite part amp(0)= ( 1.17157017996028720E-007, 2.91172237574935625E-007)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= ( 1.17157017996028720E-007, 2.91172237574935625E-007)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 6
Complete Amplitude (without r2):
finite part amp(0)= (-7.54210327705155058E-008, 1.02783630692108818E-007)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-7.54210327705155058E-008, 1.02783630692108818E-007)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 7
Complete Amplitude (without r2):
finite part amp(0)= (-3.11273119861472443E-008, 4.90795540582046004E-008)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-3.11273119861472443E-008, 4.90795540582046004E-008)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 8
Complete Amplitude (without r2):
finite part amp(0)= (-6.53258200376204763E-009,-2.15493986607851965E-008)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-6.53258200376204763E-009,-2.15493986607851965E-008)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 9
Complete Amplitude (without r2):
finite part amp(0)= (-6.80306254781754129E-007, 1.32500886416169032E-006)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-6.80306254781754129E-007, 1.32500886416169032E-006)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
iter= 10
Complete Amplitude (without r2):
finite part amp(0)= (-1.13679883442087762E-006,-1.08776236454768689E-006)
coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 )
coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 )
ampcc= (-1.13679883442087762E-006,-1.08776236454768689E-006)
R1= ( 0.0000000000000000 , 0.0000000000000000 )
stable= T
n_tot = 10.000000000000000
n_mp = 0.0000000000000000
n_unst= 0.0000000000000000
|