Abstract

We present an exploratory lattice QCD calculation of the neutrinoless double beta decay ππ→ee. Under the mechanism of light-neutrino exchange, the decay amplitude involves significant long-distance contributions. The calculation reported here, with pion masses m_{π}=420 and 140MeV, demonstrates that the decay amplitude can be computed from first principles using lattice methods. At unphysical and physical pion masses, we obtain that amplitudes are 24% and 9% smaller than the predication from leading order chiral perturbation theory. Our findings provide the lattice QCD inputs and constraints for effective field theory. A follow-on calculation with fully controlled systematic errors will be possible with adequate computational resources.

Highlights

  • Introduction.—It is a fundamental question whether the neutrinos are Dirac or Majorana-type fermions

  • According to the lightneutrino exchange mechanism, the observation of 0ν2β decay would give us information about the absolute neutrino mass, which oscillation experiments cannot predict

  • We find that the decay amplitude receives dominant long-distance contributions from the eνπ intermediate state

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Summary

Published by the American Physical Society

2 ud d4xHμνðxÞLμνðxÞ; ð3Þ where the hadronic factor HμνðxÞ 1⁄4 T1⁄2JμLðxÞJνLð0ފ with JμLðxÞ 1⁄4 u LγμdLðxÞ. While the condition of jp⃗ 1 − p⃗ 2j=kF ≪ 1 is no more valid, we target on the determination of the amplitude given in Eq (9), which is more relevant for chiral effective field theory inputs to ab initio many-body calculation [18]. We use the discrete lattice momenta ð2π=LÞm⃗ for the intermediate hadronic particles and the momenta p⃗ ν;i 1⁄4 −p⃗ i − ð2π=LÞm⃗ for the intermediate neutrino, where p⃗ i is the momentum carried by the electron. P≠ N0⃗ r) r1⁄41 of the propagator can be conφrðxÞφÃrðyÞ using the stochastic method, with φrðxÞ pffi1ffiffiffiffiffi VT q⃗ ≠0⃗ ;qt qffiqffiffitffi2ffiffiξffiþffirffiffiðffiffiqPffiffiÞffiffieffiiffiffiqiffiqffiiffixd ffiffiþffiffiffiffikffiffiffiiffi2ffi

Here the stochastic sources ξrðqÞ satisfy lim
AðgÞ þ AðeÞ
Findings
MeV MeV

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