New physics searches in neutrino experiments
Pilar Coloma
FlipPhysics Workshop
Valencia, March 25
th2022
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Do we need new physics?
Experimental evidence:
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Dark matter
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Neutrino masses
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Matter-antimatter asymmetry
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Gravitational interaction
Theoretical indications:
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Strong CP problem
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Hierarchy problem
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Flavor puzzle
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Cosmological constant
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Mass scale Coupling
strength
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Mass scale Coupling
strength
Left-Right symmetries SUSY
Leptoquarks
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Mass scale Coupling
strength
Left-Right symmetries SUSY
Leptoquarks
Heavy neutrinos Dark
matter Dark photons Axions
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Why neutrino experiments?
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Why neutrino experiments?
1) CEvNS and ν-e scattering. Field is blooming with new data thanks to advances in detector technology
2) Neutrino oscillations: at short baselines, at very long
baselines, at very different energies, in matter, in vacuum, … 3) Very powerful sources (conventional neutrino beams,
reactors, spallation sources) with near detectors
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Searches using neutrino
scattering
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Searches using neutrino scattering
+ U(1)’
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Neutrino scattering
Scattering on quarks or nuclei
Scattering
on electrons
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Coherent neutrino-nucleus scattering
Freedman, PRD 9 (1974)
In the SM:
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Neutrino scattering
Scattering on quarks or nuclei
Scattering
on electrons
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Coherent neutrino-nucleus scattering
With a Z’:
Barranco, Miranda, Rashba, hep-ph/0508299
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Scattering via a light mediator
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Experimental landscape is blooming!
Figure from Coloma, Gonzalez-Garcia, Maltoni, Pinheiro, Urrea, arXiv: 2203.XXXXX
(bounds from: Coloma, Esteban, Gonzalez-Garcia, Larizgoitia, Monrabal, Palomares-Ruiz, 2202.10829;CONUS, 2110.02174; Coloma, Gonzalez-Garcia, Maltoni, 2009.14220; CONNIE, 1910.04951;
Aliev, Bilmis, Deniz, Singh, Turan, Wong, 1502.07763)
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Searches using neutrino
oscillations
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Neutrino oscillations
Detector Source
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Neutrino oscillations
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Flavored Z’ models
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NSI in propagation
This will lead to a generalized matter potential affecting neutrino
oscillations:
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Flavored Z’ models
Coloma, Gonzalez-Garcia and Maltoni, 2009.14220
→ For sensitivities using DUNE, see yesterday’s talk by F. Capozzi
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How low in mass can we go?
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Long-range forces
See e.g. Gonzalez-Garcia, de Holanda, Masso, Zukanovich Funchal, hep-ph/0609094;
Grifols, Masso, hep-ph/0311141; Joshipura, Mohanty, hep-ph/0310210];
Davoudiasl, Lee, Marciano, 1102.5352; Wise and Zhang,1803.00591
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Long-range forces
Coloma, Gonzalez- Garcia and Maltoni 2009.14220
(see also Wise and Zhang, 1803.00591)
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Searches using neutrino beams
as fixed target experiments
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Neutrino beams
detector Far
Near detector
O(500) km
focusing horn
O(500) m
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Heavy Neutral Leptons
Figure from Snowmass 2021 White Paper on Heavy Neutral Leptons
(see references therein)
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Dark matter production
MiniBooNE coll., 1807.06137 and 1702.02688
See also e.g. Batell, Pospelov and Ritz, 0906.5614; Batell, deNIverville, McKeen, Pospelov, Ritz, 1405.7049
→
for updated NA64 results, see L. Molina’s talk!
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Milli-charged particles
Signal
Background
Harnik, Liu, Palamara, 1902.03246 For the limit from the Argoneut coll., see 1911.07996
(see also, e.g., McGill, Plestid, Pospelov, Tsai, 1806.03310)
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Axion-like particles
Coloma, Hernandez, Urrea,
2202.03447
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Axion-like particles
Brdar, Dutta, Jang, Kim, et al, 2011.07054
(see also Kelly, Kumar, Liu, 2011.05995)
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Summary and conclusions
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Neutrino experiments have a great potential to constrain new particles weakly coupled to the SM:
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Precision tests of the three-neutrino oscillation picture
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Neutrino scattering measurements
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Atmospheric production of new particles
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Fixed target searches using near detectors
→ Other scenarios not discussed here include: sterile neutrino
oscillations, neutrino decoherence, CPT violation, neutrino decay,
dark matter interactions with neutrinos…
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Thank you!!
Work supported by Grants RYC2018-024240-I PID2019-108892RB-I00, CEX2020-001007-S
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Backup slides
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Axion-like particles
Kelly, Kumar, Liu, 2011.05995
(see also Brdar, Dutta, Jang, Kim, et al, 2011.07054)