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Heavy Physics Contributions to Neutrinoless Double Beta Decay from QCD
A Nicholson1,2, E Berkowitz3, H Monge-Camacho4,5
1Department of Physics and Astronomy, University of North Carolina, Chapel Hill, North Carolina 27516-3255, USA.
Researchers computed crucial matrix elements for neutrinoless double beta decay using lattice quantum chromodynamics (QCD). This advances understanding of beyond the standard model (BSM) physics and neutrino mass nature.
Area of Science:
- Nuclear Physics
- Particle Physics
- Quantum Chromodynamics
Background:
- Neutrinoless double beta decay is a key process for understanding neutrino mass nature.
- Experimental efforts worldwide seek to observe this lepton number violating decay.
- Connecting decay rates to beyond the standard model (BSM) physics requires nonperturbative quantum chromodynamics (QCD) insights.
Purpose of the Study:
- To compute matrix elements of short-range operators contributing to neutrinoless double beta decay.
- To provide essential inputs for model-independent calculations of this decay process.
- To clarify the role of short-range operator contributions versus long-range neutrino exchange.
Main Methods:
- Lattice quantum chromodynamics (QCD) was employed to calculate matrix elements.
- Effective field theory methods were utilized in conjunction with lattice QCD results.
- Focus was on leading order π⁻→π⁺ exchange diagrams involving short-range operators.
Main Results:
- The necessary matrix elements of short-range operators were computed using lattice QCD.
- These results are crucial for understanding contributions from heavy beyond the standard model (BSM) mediators.
- Calculations indicate short-range operator contributions may rival or exceed those from long-range neutrino exchange.
Conclusions:
- The computed lattice QCD matrix elements enable model-independent calculations of two-nucleon decay.
- These findings serve as vital input for nuclear many-body calculations of experimental decays.
- Short-range operator contributions are potentially as significant as long-range neutrino exchange in neutrinoless double beta decay.
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