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The European Spallation Source Neutrino Super Beam for CP Violation discovery

Access a powerful proton beam to study CP violation through neutrino telescopes. Utilize a 5MW, 2GeV energy with 14Hz repetition rate, focusing on hadron physics. Study neutrino oscillations, atmospheric and solar interference, and potential mass hierarchy. Investigate neutrino spectra, astroparticles, and gravitational collapsing through a 500kt detector. Plan for future experiments and developments to enhance neutrino research capabilities.

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The European Spallation Source Neutrino Super Beam for CP Violation discovery

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  1. Marcos DRACOS IPHC-IN2P3/CNRS Université de Strasbourg The European Spallation Source Neutrino Super Beamfor CP Violation discovery XVI International Workshop on Neutrino Telescopes M. Dracos IPHC/CNRS-UNISTRA

  2. p Having access to a powerful proton beam… proton beam decay tunnel physics hadrons π ν • What can we do with: • 5 MW power • 2 GeV energy • 14 Hz repetition rate • 1015 protons/pulse • >2.7x1023 protons/year ⨂B target hadronic collector (focusing) Detector conventional neutrino (super) beam M. Dracos IPHC/CNRS-UNISTRA

  3. ESSνSBneutrino energy distribution anti-neutrinos neutrinos at 100 km from the target and per year (in absence of oscillations) almost pure νμ beam M. Dracos IPHC/CNRS-UNISTRA

  4. CP Violating Observables atmospheric Non-CP terms solar interference CP violating matter effect ⇒ accessibility to mass hierarchy ⇒ long baseline ≠0 ⇒ CP Violation be careful, matter effects also create asymmetry M. Dracos IPHC/CNRS-UNISTRA

  5. Neutrino Oscillations with "large" θ13 2nd oscillation maximum P(νμ→νe) 1st oscillation maximum θ13=8.8º ("large" θ13) dCP=-90 dCP=0 dCP=+90 θ13=1º ("small" θ13) L/E L/E solar atmospheric for "large" θ13 1st oscillation maximum is dominated by atmospheric term for small θ13 1st oscillation maximum is better atmospheric solar L/E L/E CP interference CP interference (arXiv:1110.4583) θ13=1º θ13=8.8º • 1st oscillation max.: A=0.3sinδCP • 2nd oscillation max.: A=0.75sinδCP more sensitivity at 2ndoscillation max. (see arXiv:1310.5992 and arXiv:0710.0554) M. Dracos IPHC/CNRS-UNISTRA

  6. Can we go to the 2nd oscillation maximum using our proton beam? Yes, if we place our far detector at around 500 km from the neutrino source. (arXiv: hep-ex/0607026) MEMPHYS Cherenkov detector (MEgaton Mass PHYSics studied by LAGUNA) • Neutrino Oscillations (Super Beam, Beta Beam) • Proton decay • Astroparticles • Understand the gravitational collapsing: galactic SN ν • Supernovae "relics" • Solar Neutrinos • Atmospheric Neutrinos • 500 kt fiducial volume (~20xSuperK) • Readout: ~240k 8” PMTs • 30% optical coverage M. Dracos IPHC/CNRS-UNISTRA

  7. Neutrino spectra below ντ production 540 km (2 GeV) neutrinos anti-neutrinos δCP=0 2 years 8 years M. Dracos IPHC/CNRS-UNISTRA

  8. 2nd Oscillation max. coverage 2nd oscillation max. well covered by the ESS neutrino spectrum 1st oscillation max. M. Dracos IPHC/CNRS-UNISTRA

  9. δCP coverage CPV (2 GeV protons) "nominal" x2 after 10 years with 2 times more statistics systematic errors (nominal values): 5%/10% for signal/background more than 50% δCP coverage using reasonable assumptions on systematic errors M. Dracos IPHC/CNRS-UNISTRA

  10. Where to find all these protons? European Spallation Source Linac M. Dracos IPHC/CNRS-UNISTRA

  11. European Spallation Source under construction phase (~1.85 B€ facility) M. Dracos IPHC/CNRS-UNISTRA

  12. ESS proton linac • The ESS will be a copious source of spallation neutrons • 5 MW average beam power • 125 MW peak power • 14 Hz repetition rate (2.86 ms pulse duration, 1015 protons) • 2.0 GeV protons (up to 3.5 GeV with linac upgrades) • >2.7x1023p.o.t/year Linac ready by 2023 (full power and energy) M. Dracos IPHC/CNRS-UNISTRA

  13. How to add a neutrino facility? • The neutron program must not be affected and if possible synergetic modifications • Linac modifications: double the rate (14 Hz → 28 Hz), from 4% duty cycle to 8%. • Accumulator (ø 143 m) needed to compress to few μs the 2.86 ms proton pulses, affordable by the magnetic horn (350 kA, power consumption, Joule effect) • H- source (instead of protons) • space charge problems to be solved • ~300 MeV neutrinos • Target station (studied in EUROν) • Underground detector (studied in LAGUNA) • Short pulses (~μs) will also allow DAR experiments neutrino flux at 100 km (similar spectrum than for EU FP7 EUROν SPL SB) M. Dracos IPHC/CNRS-UNISTRA

  14. DAR experiments(ESS/SNS) Typical expected supernova neutrino spectrum for different flavours (solid lines) and SNS/ESS neutrino spectrum (dashed and dotted lines) M. Dracos IPHC/CNRS-UNISTRA

  15. Previous Expertise M. Dracos IPHC/CNRS-UNISTRA

  16. Mitigation of high power effects(4-Target/Horn system for EUROnu Super Beam) Packed bed canister in symmetrical transverse flow configuration (titanium alloy spheres) 4-target/horn system to mitigate the high proton beam power (4 MW) and rate (50 Hz) Helium Flow target inside the horn M. Dracos IPHC/CNRS-UNISTRA

  17. General Layout of the target station(copied from EUROnu) Shield Blocks Horn Support Module Split Proton Beam Horns and Targets Collimators Decay Volume (He, 4x4x25 m3) Neutrino Beam Direction Beam Dump 8 m concrete M. Dracos IPHC/CNRS-UNISTRA

  18. Possible locations for far detector ESS Kongsberg Løkken CERN LAGUNA sites M. Dracos IPHC/CNRS-UNISTRA

  19. Which baseline? CPV MH Garpenberg Zinkgruvan • Zinkgruvan is better for 2 GeV • Garpenberg is better for > 2.5 GeV • systematic errors: 5%/10% (signal/backg.) • Zinkgruvan is better • atmospheric neutrinos are needed (at least at low energy) M. Dracos IPHC/CNRS-UNISTRA

  20. ESS Neutrino Super Beam DS arXiv:1212.5048 arXiv:1309.7022 14 participating institutes from 10 different countries, among them ESS and CERN (US "snowmass" process) M. Dracos IPHC/CNRS-UNISTRA

  21. δCP accuracy performance(USA snowmass process, P. Coloma) "default" column • for systematic errors see (7.5%/15% for ESSnuSB): • Phys. Rev. D 87 (2013) 3, 033004 [arXiv:1209.5973 [hep-ph]] • arXiv:1310.4340 [hep-ex] Neutrino "snowmass" group conclusions M. Dracos IPHC/CNRS-UNISTRA

  22. ESS Neutrino Super Beam Design Study • A H2020 Design Study has been submitted last September • 11 institutes (including ESS and CERN) from 8 European countries • Decision: • Overall score 13.5/15 (5/5 for Excellence) • not enough to be funded (only 15 MEUR for this call) • nevertheless, the evaluators recognise that ESSνSB answers one of the priorities defined in the European Strategy for Particle Physics. • New funding sources are now investigated in order to continue this design study. M. Dracos IPHC/CNRS-UNISTRA

  23. ESS under construction October 2014 M. Dracos IPHC/CNRS-UNISTRA

  24. ESS Construction near detector accumulator target station proton linac • First proton beam by 2019 • Full power/energy by 2023 February 2015 M. Dracos IPHC/CNRS-UNISTRA

  25. Muon at the level of the beam dump 2.7x1023p.o.t/year muons at the level of the beam dump (per proton) y (cm) 4.2x1020μ/year (16.3x1020 for 4 m2) x (cm) 4.1x1020μ/year 10-3 x (cm) • input beam for future 6D m cooling experiments (for muon collider) • good to measure neutrino x-sections (νμ, νe) around 200-300 MeV (low energy nuSTORM) muons/proton <Eμ>~0.46 GeV <Lμ>~2.9 km M. Dracos IPHC/CNRS-UNISTRA

  26. Conclusion • Significantly better CPV sensitivity at the 2nd oscillation maximum. • The European Spallation Source Linac will be ready in less than 10 years (5 MW, 2 GeV proton beam) • Neutrino Super Beam based on ESS linac is very promising. • ESS will have enough protons to go to the 2nd oscillation maximum and increase its CPV sensitivity. • CPV: 5 σ could be reached over 60% of δCP range (ESSνSB) with large potentiality. • Large associated detectors have a rich astroparticle physics program. • Full complementarity with a long baseline experiment on the 1st oscillation maximum using another detection technique (LAr?). M. Dracos IPHC/CNRS-UNISTRA

  27. Backup M. Dracos IPHC/CNRS-UNISTRA

  28. Neutrino Oscillations with "large" θ13 • at the 1st oscillation max.: A=0.3sinδCP • at the 2nd oscillation max.: A=0.75sinδCP 2nd oscillation maximum is better (see arXiv:1310.5992 and arXiv:0710.0554) M. Dracos IPHC/CNRS-UNISTRA

  29. Systematic errors Phys. Rev. D 87 (2013) 3, 033004 [arXiv:1209.5973 [hep-ph]] M. Dracos IPHC/CNRS-UNISTRA

  30. Systematic errors and exposure for ESSnuSB systematic errors see 1209.5973 [hep-ph] (lower limit "default" case, upper limit "optimistic" case) High potentiality P5 requirement: 75% at 3σ Neutrino Factory reach 10 years 20 years (courtesy P. Coloma) M. Dracos IPHC/CNRS-UNISTRA

  31. Effect of the unknown MH on CPV performance "default" case for systematics small effect practically no need to re-optimize when MH will be known M. Dracos IPHC/CNRS-UNISTRA

  32. Physics Performance for ESSνSB(Enrique Fernantez, Pilar Coloma) δCP precision (unknown MH) • for 2 GeV • optimum 300-400 km • for 3.5 GeV • optimum 500-600 km • but the variation is small • CPV discovery implies exclusion at 5 σ of 0º and 180º • high δCP resolution around these values is needed • 1º gain around these values increase the discovery δCP range by ~4x5x1º (1st approx.) M. Dracos IPHC/CNRS-UNISTRA

  33. Which baseline? discovery potential (unknown mass hierarchy) M. Dracos IPHC/CNRS-UNISTRA

  34. The MEMPHYS Detector(Proton decay) (arXiv: hep-ex/0607026) M. Dracos IPHC/CNRS-UNISTRA

  35. The MEMPHYS Detector(Supernova explosion) MEMPHYS SUPERK Diffuse Supernova Neutrinos (10 years, 440 kt) For 10 kpc: ~105 events M. Dracos IPHC/CNRS-UNISTRA

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