Abstract
AbstractBy an explicit calculation we demonstrate that the triple gauge-ghost vertices in a general renormalizable $${{\mathcal {N}}}=1$$
N
=
1
supersymmetric gauge theory are UV finite in the two-loop approximation. For this purpose we calculate the two-loop divergent contribution to the $$\bar{c}^+ V c$$
c
¯
+
V
c
-vertex proportional to $$(C_2)^2$$
(
C
2
)
2
and use the finiteness of the two-loop contribution proportional to $$C_2 T(R)$$
C
2
T
(
R
)
which has been checked earlier. The theory under consideration is regularized by higher covariant derivatives and quantized in a manifestly $${{\mathcal {N}}}=1$$
N
=
1
supersymmetric way with the help of $${{\mathcal {N}}}=1$$
N
=
1
superspace. The two-loop finiteness of the vertices with one external line of the quantum gauge superfield and two external lines of the Faddeev–Popov ghosts has been verified for a general $$\xi $$
ξ
-gauge. This result agrees with the nonrenormalization theorem proved earlier in all orders, which is an important step for the all-loop derivation of the exact NSVZ $$\beta $$
β
-function.
Funder
Foundation for the Advancement of Theoretical Physics and Mathematics
Publisher
Springer Science and Business Media LLC
Subject
Physics and Astronomy (miscellaneous),Engineering (miscellaneous)
Cited by
6 articles.
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