-
[1]
T. Hahn, S. Paßehr, and C. Schappacher, PoS LL2016, 068 (2016), arXiv:1604.04611[hep-ph
-
[2]
J. Alwall, R. Frederix, S. Frixione et al., JHEP 07, 079 (2014), arXiv:1405.0301[hep-ph
-
[3]
W. Kilian, T. Ohl, and J. Reuter, Eur. Phys. J. C 71, 1742 (2011), arXiv:0708.4233[hep-ph
-
[4]
G. Cullen et al., Eur. Phys. J. C 74, 3001 (2014), arXiv:1404.7096[hepph
-
[5]
G. Belanger, F. Boudjema, J. Fujimoto et al., Phys. Rept. 430, 117 (2006), arXiv:hep-ph/0308080
-
[6]
S. Borowka, G. Heinrich, S. P. Jones et al., Comput. Phys. Commun. 196, 470 (2015), arXiv:1502.06595[hepph
-
[7]
S. Borowka, G. Heinrich, S. Jahn et al., Comput. Phys. Commun. 222, 313 (2018), arXiv:1703.09692[hepph
-
[8]
A. V. Smirnov, Comput. Phys. Commun. 204, 189 (2016), arXiv:1511.03614[hep-ph
-
[9]
A. V. Smirnov and F. S. Chuharev, Comput. Phys. Commun. 247, 106877 (2020), arXiv:1901.07808[hep-ph
-
[10]
X. Liu and Y.-Q. Ma, AMFlow: a Mathematica package for Feynman integrals computation via Auxiliary Mass Flow, (2022), arXiv: 2201.11669[hep-ph]
-
[11]
T. Horiguchi, A. Ishikawa, T. Suehara et al., Study of top quark pair production near threshold at the ILC, (2013), arXiv: 1310.0563[hep-ex]
-
[12]
M. S. Amjad et al., Eur. Phys. J. C 75, 512 (2015), arXiv:1505.06020[hep-ex
-
[13]
K. Seidel, F. Simon, M. Tesar et al., Eur. Phys. J. C 73, 2530 (2013), arXiv:1303.3758[hepex
-
[14]
H. Abramowicz et al. (CLICdp), JHEP 11, 003 (2019), arXiv:1807.02441[hep-ex
-
[15]
J. Fuster, I. García, P. Gomi et al., Eur. Phys. J. C 75, 223 (2015), arXiv:1411.2355[hep-ex
-
[16]
R. Vega and J. Wudka, Phys. Rev. D 53, 5286 (1996), [Erratum: Phys. Rev. D 56, 6037–6038 (1997)], arXiv: hepph/9511318
-
[17]
C.-H. Chang and Y.-Q. Chen, Phys. Rev. D 46, 3845 (1992), [Erratum: Phys. Rev. D 50, 6013 (1994)]
-
[18]
A. L. Bondarev, Methods of minimization of calculations in high-energy physics: 1. A covariant method for calculating amplitudes of processes involving polarized Dirac particles, (1997), arXiv: hep-ph/9710398
-
[19]
C.-F. Qiao, Phys. Rev. D 67, 097503 (2003), arXiv:hepph/0302128
-
[20]
Z.-Q. Chen and C.-F. Qiao, The trace amplitude method and its application to the NLO QCD calculation, (2021), arXiv: 2101.01106[hep-ph].
-
[21]
F. A. Berends, R. Kleiss, P. De Causmaecker et al., Phys. Lett. B 103, 124 (1981)
-
[22]
P. De Causmaecker, R. Gastmans, W. Troost et al., Nucl. Phys. B 206, 53 (1982)
-
[23]
R. Kleiss and W. J. Stirling, Nucl. Phys. B 262, 235 (1985)
-
[24]
R. Gastmans and T. T. Wu, The Ubiquitous photon: Helicity method for QED and QCD, Vol. 80 (1990)
-
[25]
Z. Xu, D.-H. Zhang, and L. Chang, Nucl. Phys. B 291, 392 (1987)
-
[26]
J. F. Gunion and Z. Kunszt, Phys. Lett. B 161, 333 (1985)
-
[27]
K. Hagiwara and D. Zeppenfeld, Nucl. Phys. B 274, 1 (1986)
-
[28]
R. Britto, F. Cachazo, and B. Feng, Nucl. Phys. B 715, 499 (2005), arXiv:hep-th/0412308
-
[29]
R. Britto, F. Cachazo, B. Feng et al., Phys. Rev. Lett. 94, 181602 (2005), arXiv:hepth/0501052
-
[30]
C. Schwinn and S. Weinzierl, JHEP 05, 006 (2005), arXiv:hep-th/0503015
-
[31]
C. Schwinn and S. Weinzierl, JHEP 03, 030 (2006), arXiv:hep-th/0602012
-
[32]
C. Schwinn and S. Weinzierl, JHEP 04, 072 (2007), arXiv:hep-ph/0703021
-
[33]
N. Craig, H. Elvang, M. Kiermaier et al., JHEP 12, 097 (2011), arXiv:1104.2050[hep-th
-
[34]
R. H. Boels and C. Schwinn, Phys. Rev. D 84, 065006 (2011), arXiv:1104.2280[hep-th
-
[35]
N. Arkani-Hamed, T.-C. Huang, and Y.-t. Huang, JHEP 11, 070, arXiv: 1709.04891[hep-th]
-
[36]
R. Aoude and C. S. Machado, JHEP 12, 058, arXiv: 1905.11433[hep-ph]
-
[37]
S. Ballav and A. Manna, JHEP 03, 295, arXiv: 2010.14139[hep-th]
-
[38]
A. Herderschee, S. Koren, and T. Trott, JHEP 08, 107, arXiv: 1902.07205[hep-th]
-
[39]
R. Franken and C. Schwinn, JHEP 02, 073, arXiv: 1910.13407[hep-th].
-
[40]
J.-X. Wang, Nucl. Instrum. Meth. A 534, 241 (2004), arXiv:hep-ph/0407058
-
[41]
M. Moretti, T. Ohl, and J. Reuter, O’Mega: An Optimizing matrix element generator, (2001), arXiv: hepph/0102195
-
[42]
W. Kilian, T. Ohl, and J. Reuter, private communication