Approaching the neutrino mass problem with the DUNE Near Detector - - PowerPoint PPT Presentation

approaching the neutrino mass problem
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Approaching the neutrino mass problem with the DUNE Near Detector - - PowerPoint PPT Presentation

11th June 2019 INVISIBLES19 Workshop Approaching the neutrino mass problem with the DUNE Near Detector Peter Ballett, Tommaso Boschi , Silvia Pascoli tommaso.boschi@durham.ac.uk Durham University Institute for Particle Physics Phenomenology


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11th June 2019 INVISIBLES’19 Workshop

Approaching the neutrino mass problem

with the DUNE Near Detector

Peter Ballett, Tommaso Boschi, Silvia Pascoli tommaso.boschi@durham.ac.uk

Durham University Institute for Particle Physics Phenomenology

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Approaching the neutrino mass problem

with the DUNE Near Detector

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Approaching the neutrino mass problem

with the DUNE Near Detector

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Neutrino mass problem

ν-fit 4.0 [2018] ∆m2

21 = 7.39+0.21 −0.20 × 10−5 eV2

|∆m2

31| = 2.522+0.033 −0.031 × 10−3 eV2

Plank [2018]

  • i

mνi < 0.12 eV Troitsk [2011] with 3H β-decay

  • i

|Uei|2mνi < 2.05 eV

Problems: No νR in SM, so no Yukawa (d ≤ 4) mν ≪ me, six orders of magnitude! ν can be a Majorana particle... The solution can be theoretically easy: just add heavy neutrinos, or Heavy Neutral Leptons, to SM! But this is phenomenologically/experimentally hard, e.g. Type I seesaw typically requires new particles at GUT scale.

Tommaso Boschi UDUR, IPPP 2

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Approaching the Heavy Neutral Leptons

with the DUNE Near Detector

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Approaching the Heavy Neutral Leptons

with the DUNE Near Detector

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Testable signatures

A symmetry-protected seesaw can lower the physics scale! “Recipe” for a low-scale seesaw Extend the SM by adding singlet fermions Ni with LN = +qL and Si with LN = −qL. Majorana mass terms, with “natural” LNV parameters and cancellations among high scale contributions. Lightness of neutrino mass is described, but also heavier new particles: HNL. Forbidden mixing angles and HNL masses accessible by current and future experiment can be reached. Sterile neutrinos mix with light neutrinos into flavour neutrinos |να =

  • i

Uαi |Ni New particles take part to any process in which neutrinos are involved. Inverse seesaw M =   mT

D

mD µR MT

R

MR µS   Signature: lightest HNL is produced in a neutrino beam and then decays into charged particles.

Tommaso Boschi UDUR, IPPP 3

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Heavy Neutral Leptons from low-scale seesaws

with the DUNE Near Detector

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Heavy Neutral Leptons from low-scale seesaws

with the DUNE Near Detector

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DUNE Near Detector

Main goal is precision oscillation physics, but also large variety of complementary studies. Near Detector is required to normalise flux and remove cross-section systematics. ND system (current design) LArTPC with fiducial volume 24 m3 and mass 35 t. Multi Purpose Detector (MPD), which is a gaseous TPC, fiducial volume 100 m3 and mass 1 t. LArTPC and MPD are movable (DUNE-PRISM). 3D Scintillation Tracker, on-axis, for flux monitoring and neutron contamination.

Tommaso Boschi UDUR, IPPP 4

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The neutrino mass problem has numerous solutions, some of them can be tested in current/future experiments, like Inverse seesaw. The experimental signature is decay in-flight of an HNL. Different realisations of the model are reflected in different phenomenology. The DUNE Near Detector has the perfect features to help tackle this problem

Can we approach the neutrino mass problem with the DUNE Near Detector?

  • Maybe. Come check my poster!