electromagnetic interactions of neutrinos in matter int. school of nuclear physics probing hadron...
TRANSCRIPT
![Page 1: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/1.jpg)
ELECTROMAGNETIC INTERACTIONS OF
NEUTRINOS IN MATTER
Int. School of Nuclear PhysicsProbing hadron structure with lepton & hadron beams
![Page 2: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/2.jpg)
E.M. interactions of neutrinos
1) Radiative decays
2) Magnetic moment
3) Stimulated conversion … all GIM suppressed in
vacuum!
2 1W
l
![Page 3: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/3.jpg)
Present limits
Radiative decaysSM theory: 0 = 7 1043 (1eV/m)5 (s) Pal & Wolfenstein (1982)
Experiments: SN1987 (strong MH): /m > 6 1015 s/eV Bugey (mass degenerated): m > 310-4 s/eV if m/m >10-7
Solar eclipse : m > 100 s/eV if m2 ~ 10-5 eV2
Magnetic momentSM theory: = 3.2 10-19 m(eV) B
Experiment (solar): < 0.54 10-10 B
![Page 4: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/4.jpg)
Amplification in matter
Coherent interactions on the atomic electrons
e
2
W
1
e
0/m ~ 9 1023 F(v)(Ne/1024cm-3)2 (1eV/m)4
If mass-degenerated
0/m ~ 9 1023 F(v)(Ne/1024cm-3)2 (1eV/m)4 (m2/m2)2
J.C.d’Olivo, J.F.Nieves (1989), G.Giunti et al. (1991)
![Page 5: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/5.jpg)
Neutrino energy deposition in a Ge crystal
Neutrino beam
High purity Ge diode 140 cm3 at liquid nitrogen temperature (77K)Electron-hole pair creation work 3 eV: very low
energy thresholdEnergy resolution ~ keV
![Page 6: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/6.jpg)
Integral search: the principleA.Castera et al., Phys.Lett.B452, 150
High intensity beam: 20 GeV 1013 pot in 4 ms spills, every 14 s
1 mip (muon) gives a sudden signal~ 30 MeV in 5 cm
Search: Continuous energy deposition building up during the spill duration
![Page 7: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/7.jpg)
Results
Clear on-beam signal of crossing mip’s
No excess of deposited energy < 3 keV in 5 cm
![Page 8: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/8.jpg)
Analysis8 107 and anti- per spill crossing the crystal
Total energy deposition < 3 keV in 5 cm of Ge
< 10-5 eV /cm: 10-12 normal dE/dx< 10 keV for whole earth diameter~ 10-2 eV /cm for weak interactions
Case of mass-degenerated radiative decayE = E m2/m2 = E 2m/m 2 eV < E < 200
eV10-10 < m/m < 10-8
Prob < 10-5/E m > 5/3 10-5 m2/m0 > 1.5 1018 m3/m2
![Page 9: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/9.jpg)
An encore at the Bugey reactor
Powerful source of anti-e: ~ 1021/sBut also e from activation of the container: 55Fe produces a peak at 230 keV and 51Cr peak at 750 keV15 m from the core: 4 109 /cm2 for each of the 2 peaks
m/m > 3 10-4 s/eV in Geequivalent to
/m > 9 1015 s/eV in vacuum
![Page 10: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/10.jpg)
Stimulated conversion in an RF cavityAnother way to amplify EM interactions M.C Gonzalès-Garcia, F. Vannucci and J. Castromonte Phys.Lett. B373,153(1996)
Idea: an RF cavity is a photon bath (100W 109 QF~1023 cm3 à 10-6 eV)
Majorana neutrinos anti-e ou anti-
Dirac neutrinos sterile
R = N/N = (Q/109)(P/100W)(m/eV)3(eV2/m2)3(s/)
0 = 20/R (m/m2)3
If R<10-2 0 > 2 1018s for m2=10-5 eV2 and m=1 eV
But also + +
![Page 11: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/11.jpg)
Recent development: sterile neutrinos
What are sterile neutrinos?-Do not participate in Weak Interactions-Couple to the “real world” through mixing
(e, , , H …) = [U] (1, 2, 3, 4 …)
Bad reasons: try to explain anomalies in past neutrino dataLSND, MiniBoone, nuclear reactors, radioactive sources
Good reasons: neutrinos are massive, need of Right Handed componentsClassical see-saw model, very high masses, but variations exist
Every neutrino flux has some H component at the level of UHl2
![Page 12: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/12.jpg)
Example: the MSM modelThree sterile neutrinos, one of them having ~10 keV/c2 mass
Almost stable DARK MATTER
• Warm Dark Matter
7 1043 (1eV/m)5(1/U2) (s)
![Page 13: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/13.jpg)
Cosmological limits
Search of monoenergetic photons
![Page 14: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/14.jpg)
Sterile neutrinos as WDMm(H) ~ 7 keVU2 ~ 10-10
In vacuum:0 = 4 1034 sIn matter:m ~1026 s
Local Dark Matter density: 300 MeV/cm3
Relative velocity: 200 km/sFlux of H on earth: 8 1011 H/cm2s (yearly modulation)
In crystal 1x1x1 m3: 10-8 decay/year !!… 5 10-4/year in SK, 10/year in IceCube
![Page 15: ELECTROMAGNETIC INTERACTIONS OF NEUTRINOS IN MATTER Int. School of Nuclear Physics Probing hadron structure with lepton & hadron beams](https://reader030.vdocuments.us/reader030/viewer/2022032709/56649eb75503460f94bc0b84/html5/thumbnails/15.jpg)
Conclusion
EM neutrino interactions exist in the Standard Model-Recent claim in astrophysics of radiative decay
indication?
They are hugely amplified in matter
… but not yet enough to consider an experiment in the labUnless nuclear physics help?