Decoupling relations to O(α s3) and their connection to low-energy theorems
If quantum chromodynamics (QCD) is renormalized by minimal subtraction (MS), at higher orders, the strong coupling constant α s and the quark masses m q exhibit discontinuities at the flavour thresholds, which are controlled by so-called decoupling constants, ζ g and ζ m , respectively. Adopting the...
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Published in | Nuclear physics. B Vol. 510; no. 1; pp. 61 - 87 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
1998
|
Subjects | |
Online Access | Get full text |
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Summary: | If quantum chromodynamics (QCD) is renormalized by minimal subtraction (MS), at higher orders, the strong coupling constant
α
s
and the quark masses
m
q
exhibit discontinuities at the flavour thresholds, which are controlled by so-called decoupling constants,
ζ
g
and
ζ
m
, respectively. Adopting the modified MS (
MS
) scheme, we derive simple formulae which reduce the calculation of
ζ
g
and
ζ
m
to the solution of vacuum integrals. This allows us to evaluate
ζ
g
and
ζ
m
through three loops. We also establish low-energy theorems, valid to all orders, which relate the effective couplings of the Higgs boson to gluons and light quarks, due to the virtual presence of a heavy quark
h, to the logarithmic derivatives with respect to
m
h
, of
ζ
g
and
ζ
m
, respectively. Fully exploiting the present knowledge of the anomalous dimensions of
α
s
and
m
q
, we thus calculate these effective couplings through four loops. Finally, we perform a similar analysis for the coupling of the Higgs boson to photons. |
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ISSN: | 0550-3213 1873-1562 |
DOI: | 10.1016/S0550-3213(98)81004-3 |