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Presentation transcript:

http://vietnam.in2p3.fr/2019/neutrinos/index.html

XVth Rencontres du Vietnam 2019: Three Neutrinos and Beyond The theme of the meeting will be based on the 30th anniversary of the first collisions in SLC (April 1989) and LEP (August 1989), which was followed very quickly by the discovery that there are only three families of light active neutrinos The program will address the present status of neutrino properties and oscillations and beyond: the searches towards the understanding of the origin of neutrinos masses and its consequences (in particular leptogenesis and why we exist at all).

Concluding remarks. 1. goals of the meeting 2. the main questions 1989 3 neutrinos (nue,numu,nutau) if it had not been for the discovery of oscillations, this might have been the end of neutrino physics no!because of the solar neutrino problem... 3. origin of masses the status of the mass hierarchy the importance of T2K+NOvA, JUNO, SK+GD & ICECUBE ORCA 4. CP violation the status of CP violation 5. the near future we can predict that the hierarchy will be known soon from T2K+NOvA, more data from ICECUBE, data from SK-Gd, then JUNO, ORCA, then DUNE. 6. the longer future HyperK, DUNE, more huge project such as ORCA+Protvino etc.. the need for more neutrino interaction study new beams, EnuBET and nuSTORM --> need to work on the customers and synergies! 7. the origin of neutrino masses neutrinos have mass --> new physics yukawa coupling = mass term --> RH neutrinos (chirality!) Majorana mass term by Weinberg operator --> but what is the scale? NB we do not understand the Yukawa masses but at least we know them. more or less any scale above pion mass can do the job of matter asymmetry the dark matter with one particle requires 1-100 keV mass range. other related topic might give us more hints 8. neutrinoless double beta decay (fermion number violation) 9. search for right-handed neutrinos eV sterile neutrino beware the sigmas when there are assumptions! heavy neutral leptons new generation of hadron experiments hadron collider experiments e+e- Z factory, precision measurements & tau decays the long lived region. the high energy region --> very difficult! 10. the heavy neutrino search in hadron colliders is a new experiment! new trigger, new detector optimization at least one FCC detector to be optimized for RH neutrino search! 11. BIG REMARKS -- we are nearing the time when the neutrino oscillation phenomenon will be entirely specified (mass hierarchy CP phase, octant) -- what will neutrino physics become then? -- mass scale (compare KATRIN results with ccosmological) -- however we need unambiguous mass measurement (how? more of KATRIN, Project 8, etc...) -- the topic will certainly move to search for origin of neutrino masses -- maybe the easiest of the 'search for origin of particle mass' questions. -- a Z factory seems the most straight forward solution -- one or several HUGE neutrino-less double beta decay experiment? 12 thanks the organizers -- parallel sessions became serial sessions!

new data this year main result: normal mass ordering is very much preferred at 2 = 10.4 (3.2 sigma) NB this is quite significant for such a well-defined predefined bimodal test! (many argue that 5 sigma not needed) NBB note importance of atmospheric (SK) watch T2K+NOvA, ICECUBE, SK+GD, ORCA… ... DUNE (matter effect) JUNO (direct dephasing meast) it should not take long before the question is solved!

With the data we have today (175 ee events) -- Mass Ordering is nearly surely normal -- the measurement of the CPV phase CP = - (41 -28 +39)o still ways to go. careful: error depends on value. -- sensitivity to octant comes from e appearance (sensitive to sin2 23 ) this issue (and its relevance) will simply disappear in the near future with more statistics.

Gd in SuperK! improve sensitivity to -- relic SN neutrinos -- atmospherics ( MO and CPV) -- T2K beam (esp. run!)

Another cornerstone -oscillation experiment (MO from phase measurement, not matter effect)

HYPERK and DUNE are now on orbit  2027! main mission: measurement of CP and test of CP violation+ many oter things incl. p decay! They will measure CP to precison depending on value… but CPV discovery not guaranteed! Quality of the results will be conditionned by measurements of (anti) e vs  cross-sections and properties (energy shifts in particular)  EnuBET/NUSTORM + hadrop. exp. NA61

where are the right-handed neutrinos? 3 neutrinos and beyond it is a daily observation that neutrinos are leaning to the left: where are the right-handed neutrinos? neutrino Yukawa coupling  RH neutrino exists + if Majorana mass term exists (matter  antimatter transition)  mass splitting and mixing NB in see-saw all neutrinos are Majorana particles with mixing btw. left and right-handed NBB terminology refers to the chirality of the particle (not the helicity) NBBB in the weak interaction, right-handed is equivalent to sterile

Deppisch showed us that signal  Majorana mass term However Majorana mass term may (accidentally) not give a signal

It is a novelty of this meeting that so much emphasis was given to the searches for right-handed (or sterile) neutrinos. It is a novelty of the time that so much attention is paid by the high energy physics community to this search -- eV scale neutrino oscillation experiments (reactor, short and long baseline) -- BELLE/BELLE II, ATLAS&CMS, LHCb, FASER, MATHUSLA -- NA62, NA64, SHIP…. one family see-saw  ||2 = mv/mN eV scale mv = 50 meV neutrino  ||2 = 0.05 for mN = 1 eV (this is ~ the LSND value, but this one is ‘ruled out by disappearance expts.) However we do not know that mv is 50 meV ||2 down to 0.01 (0.08) is excluded for  (resp e ) there is plenty of space left for another sterile neutrino in that mass range!  in three family see-saw ||2  mv/mN

SB expts..

In general these experiments offer many opportunities!

Alain Blondel FCC CDR presentation Outlook Heavy neutrinos FCC-ee Z or 𝑙 + (*) FCC-hh - FCC-ee -- EWPO : sensitivity 10-5 up to very high masses -- high sensitivity to single N( 𝑙2 W) in Z decay FCC-hh -- production in W-> 𝑙1 + N( 𝑙2 W) with initial and final lepton charge and flavour FCC e-p -- production in CC e p  X N( 𝑙W) high mass Complementarity: discovery + studies of FNV and LFV! Detached vertices The capability to probe massive neutrino mechanisms for generating the matter-antimatter asymmetry in the Universe should be a central consideration in the selection and design of future colliders. (from the neutrino town meeting report to the ESPP) 30.10.2019 Alain Blondel FCC CDR presentation Outlook

Parallel sessions (3-6 hrs each) Serial Present status of neutrino oscillations and future prospects Convener Son Cao + Tsuyoshi Nakaya (include cross-section issues) 2. Experimental searches for sterile/RH/HNL/Majorana neutrinos Conveners B. Kayser and Joachim Kopp neutrino beams, astronomy, beam dumps, colliders 3. Other manifestations of neutrino mass models Conveners Martin Hirsch and Marcin Chrząszcz  neutrinoless double beta decay, manifestations of LFV and LNV, LUV, proton decay… 4. experimental techniques Conveners Davide Sgalaberna + Ornella Palomara

Program committee Jacques Dumarchez Marcin Chrząszcz Raj Gandhi Boris Kayser Manfred Lindner Sotiris Loucatos Tsuyoshi Nakaya Ornella Palomara Davide Sgalaberna

Son Cao and Tran Than Van Let us wish success to Son Cao and Tran Than Van in establishing a neutrino group in Quy Nhon!