scholarly journals Four-loop QCD propagators and vertices with one vanishing external momentum

2017 ◽  
Vol 2017 (6) ◽  
Author(s):  
B. Ruijl ◽  
T. Ueda ◽  
J. A. M. Vermaseren ◽  
A. Vogt
Keyword(s):  
2020 ◽  
Vol 80 (7) ◽  
Author(s):  
B. Ananthanarayan ◽  
Samuel Friot ◽  
Shayan Ghosh

Abstract We derive new convergent series representations for the two-loop sunset diagram with three different propagator masses $$m_1,\, m_2$$m1,m2 and $$m_3$$m3 and external momentum p by techniques of analytic continuation on a well-known triple series that corresponds to the Lauricella $$F_C^{(3)}$$FC(3) function. The convergence regions of the new series contain regions of interest to physical problems. These include some ranges of masses and squared external momentum values which make them useful from Chiral Perturbation Theory to some regions of the parameter space of the Minimal Supersymmetric Standard Model. The analytic continuation results presented for the Lauricella series could be used in other settings as well.


2007 ◽  
Vol 22 (12) ◽  
pp. 903-914 ◽  
Author(s):  
A. ABADA ◽  
K. BOUAKAZ ◽  
D. DEGHICHE

We calculate the fermion damping rates to second order in powers of the external momentum in the context of QED at finite temperature using the hard-thermal-loop summation scheme. We find the coefficients of zeroth and first orders finite whereas that of second-order logarithmically infrared sensitive. The calculation is done in covariant gauge and the result is independent of gauge fixing.


1999 ◽  
Vol 14 (27) ◽  
pp. 4331-4345 ◽  
Author(s):  
R. DELBOURGO ◽  
DONGSHENG LIU ◽  
M. D. SCADRON

We show that all abnormal parity three-body meson interactions can be adequately described by quark loops, evaluated at zero external momentum, with couplings determined by U(Nf) symmetry. We focus primarily on radiative meson decays which involve one pseudoscalar. The agreement with experiment for nonrare decays is surprisingly good and requires very few parameters, namely the coupling constants gπqq and gρqq and some mixing angles. This agreement extends to some three-body decays that are dominated by pion pairs in a P-wave state.


2016 ◽  
Vol 31 (27) ◽  
pp. 1650153
Author(s):  
J. S. N. Furtado ◽  
G. R. Silva

In this work, we study the generation of a nonlinear correction for QED, namely, the Euler–Heisenberg effective action. In order to achieve this, we consider two methods. The first method employed consists in make use of Feynman parametrization to solve the integrals properly, while in the second method a derivative expansion in the external momentum was considered.


2017 ◽  
Vol 12 (0) ◽  
pp. 1203039-1203039 ◽  
Author(s):  
Masanori NUNAMI ◽  
Masahiko SATO ◽  
Motoki NAKATA ◽  
Shinichiro TODA ◽  
Hideo SUGAMA ◽  
...  

2002 ◽  
Vol 17 (28) ◽  
pp. 4113-4132 ◽  
Author(s):  
J. PESTIEAU ◽  
C. SMITH

A simple method to compute QED bound state properties is presented, in which binding energy effects are treated nonperturbatively. It is shown that to take the effects of all ladder Coulomb photon exchanges into account, one can simply perform the derivative of standard QED amplitudes with respect to the external momentum. For example, the derivative of the light-by-light scattering amplitude gives an amplitude for orthopositronium decay to three photons where any number of Coulomb photon exchanges between the e+e-is included.Various applications are presented. From them, it is shown that binding energy must be treated nonperturbatively in order to preserve the analyticity of positronium decay amplitudes.Interesting perspectives for quarkonium physics are briefly sketched.


2010 ◽  
Vol 17 (5) ◽  
pp. 056108 ◽  
Author(s):  
W. M. Solomon ◽  
K. H. Burrell ◽  
A. M. Garofalo ◽  
S. M. Kaye ◽  
R. E. Bell ◽  
...  

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