Related Experiment Video
Updated: Jul 16, 2026

Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
Two-loop virtual top-quark effect on Higgs-boson decay to bottom quarks
Mathias Butenschön1, Frank Fugel, Bernd A Kniehl
1II. Institut für Theoretische Physik, Universität Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany.
The study details the dominant two-loop electroweak correction to the Higgs boson decaying into bottom quarks. This correction significantly amplifies previous findings, enhancing the decay width beyond strong-interaction screening effects.
Area of Science:
- High Energy Physics
- Particle Physics
- Quantum Field Theory
Background:
- The Standard Model Higgs boson is a fundamental particle.
- Higgs boson decays are crucial for understanding particle physics.
- Previous studies identified one-loop corrections to Higgs decays.
Purpose of the Study:
- To calculate the dominant two-loop electroweak correction to the Higgs boson decay width into bottom quarks.
- To analyze the impact of these corrections on the decay width.
- To compare electroweak corrections with strong-interaction effects.
Main Methods:
- Analytic calculation of two-loop electroweak corrections.
- Perturbative quantum field theory techniques.
- Evaluation of terms of order O(GF^2*m_t^4).
Main Results:
- The dominant two-loop electroweak correction amplifies the decay width.
- This amplification is approximately +16%, exceeding the one-loop correction.
- The two-loop effect compensates for strong-interaction screening (-8%).
Conclusions:
- Two-loop electroweak corrections are significant for Higgs boson decays to bottom quarks.
- These corrections play a vital role in precise predictions for the Standard Model.
- The findings refine our understanding of Higgs boson properties and interactions.
More Related Videos
Related Concept Videos
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Thomson's e/m Experiment
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The magnetic...
Detection of Black Holes
Their closest cousins are neutron stars, which are composed almost entirely of neutrons packed against each other, making them extremely dense. A neutron star has the same mass as the Sun but its diameter is only a few kilometers. Therefore, the escape velocity from their surface is close to the speed of light.
Not until the 1960s, when the first neutron...
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
Fermi Level
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
Double Resonance Techniques: Overview
Spin decoupling is usually achieved by...

