Abstract

We compute three-loop corrections to the Higgs-gluon form factor, incorporating the top quark mass dependence. Our method is based on the combination of expansions around the top threshold and for large top quark mass, using conformal mapping and Pad\'e approximation to describe the form factor over the full kinematic range.

Highlights

  • − ð99 − 6nlÞlog2ð1 − zފð1 − zÞ þ Oðð1 − zÞ3=2Þ; ð1Þ with Ls 1⁄4 logð−4z − i0Þ

  • Note that the additional term is proportional to ðLs − 2 ln 2Þ 1⁄4 −iπ þ Oð1 − zÞ and does not affect the real part of the coefficient

  • We find that it is no longer required to enhance the exclusion region for the coefficient of Ls for FðΔ2;0Þ;finðzÞ to Eq (14) in this paper

Read more

Summary

Introduction

− ð99 − 6nlÞlog2ð1 − zފð1 − zÞ þ Oðð1 − zÞ3=2Þ; ð1Þ with Ls 1⁄4 logð−4z − i0Þ. Note that the additional term is proportional to ðLs − 2 ln 2Þ 1⁄4 −iπ þ Oð1 − zÞ and does not affect the real part of the coefficient. Ð3 þ pffiffiffiffiffiffiffiffiffiffi π2Þ 1 − z þ π2 54 − ð99 − 6nlÞlog2ð1 − zފð1 − zÞ þ Oðð1 − zÞ3=2Þ; ð1Þ

Results
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call