Abstract:For the vertex corrections to the partial decay rate Γ(Z → bb) involving the top quark only the leading terms of order αα s in the 1/M t expansion are known. In this work we compute the missing next-to-leading corrections. Thus at O(αα s ) the complete corrections to the decay of the Z boson into bottom quarks are at hand.
“…The general result for the two-loop order β e is known [1] and for the three-loop order contributions we find (generalising the QCD results from Ref. [2], using a similar calculational setup to the one applied in [1,2], which relies on the computer programs QGRAF [15], q2e, exp [16,17] and MINCER [18]): …”
We present four-loop results for the gauge β-function and the fermion mass anomalous dimension for a gauge theory with a general gauge group and a multiplet of fermions transforming according to an arbitrary representation, calculated using the dimensional reduction scheme. In the special case of a supersymmetric theory we confirm previous calculations of both the gauge β-function and the gaugino mass β-function.
“…The general result for the two-loop order β e is known [1] and for the three-loop order contributions we find (generalising the QCD results from Ref. [2], using a similar calculational setup to the one applied in [1,2], which relies on the computer programs QGRAF [15], q2e, exp [16,17] and MINCER [18]): …”
We present four-loop results for the gauge β-function and the fermion mass anomalous dimension for a gauge theory with a general gauge group and a multiplet of fermions transforming according to an arbitrary representation, calculated using the dimensional reduction scheme. In the special case of a supersymmetric theory we confirm previous calculations of both the gauge β-function and the gaugino mass β-function.
“…The rules of asymptotic expansion (see, e.g., Ref. [24]) are applied on a diagrammatic level using exp [25,26] and finally we evaluate the resulting vacuum integrals which (after asymptotic expansion) only contain a single scale with the help of the package MATAD [27]. The automated setup allows us to perform the calculation for general gauge parameter ξ. Whereasζ 1 ,ζ 3 and ζ 3 individually depend on ξ it drops out in the combination for ζ αs which serves as a welcome check for our calculation.…”
Section: Decoupling Of Heavy Supersymmetric Particlesmentioning
We compute the three-loop QCD corrections to the decoupling constant for α s which relates the Minimal Supersymmetric Standard Model to Quantum Chromodynamics with five or six active flavours. The new results can be used to study the stability of α s evaluated at a high scale from the knowledge of its value at M Z . We furthermore derive a low-energy theorem which allows the calculation of the coefficient function of the effective Higgs boson-gluon operator from the decoupling constant. This constitutes the first independent check of the matching coefficient to three loops.
“…[25]. The various diagram topologies are identified and transformed to FORM [26] with the help of q2e and exp [27,28]. The program exp is also used in order to apply the asymptotic expansion (see, e.g., Ref.…”
Section: The Higgs Boson Mass In the Mssmmentioning
Within the minimal supersymmetric extension of the Standard Model, the mass of the light CP-even Higgs boson is computed to three-loop accuracy, taking into account the next-to-next-toleading order effects from supersymmetric Quantum Chromodynamics. We consider two different scenarios for the mass hierarchies of the supersymmetric spectrum. Our numerical results amount to corrections of about 500 MeV which is of the same order as the experimental accuracy expected at the CERN Large Hadron Collider (LHC).
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