Search for sterile neutrinos with SOX: Monte Carlo studies of the experiment sensitivity Davide Basilico 1st year Workshop – 11/10/17 Tutors: Dott. Barbara.

Slides:



Advertisements
Similar presentations
Results from Daya Bay Xin Qian On behalf of Daya Bay Collaboration Xin Qian, BNL1.
Advertisements

Sensitivity of the DANSS detector to short range neutrino oscillations
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
1 Deep Sea Neutrino Telescope Detection Principle.
Source Neutrino Experiments
Prospects for 7 Be Solar Neutrino Detection with KamLAND Stanford University Department of Physics Kazumi Ishii.
Experimental Status of Geo-reactor Search with KamLAND Detector
Reactor & Accelerator Thanks to Bob McKeown for many of the slides.
Results and Future of the KamLAND Experiment
Neutrino emission =0.27 MeV E=0.39,0.86 MeV =6.74 MeV ppI loss: ~2% ppII loss: 4% note: /Q= 0.27/26.73 = 1% ppIII loss: 28% Total loss: 2.3%
LENA Low Energy Neutrino Astrophysics L. Oberauer, Technische Universität München LENA Delta EL SUD Meeting.
A long baseline neutrino oscillation search - MINOS Reinhard Schwienhorst School of Physics and Astronomy University of Minnesota.
Atmospheric Neutrino Oscillations in Soudan 2
1 The Daya Bay Reactor Electron Anti-neutrino Oscillation Experiment Jianglai Liu (for the Daya Bay Collaboration) California Institute of Technology APS.
The Elementary Particles. e−e− e−e− γγ u u γ d d The Basic Interactions of Particles g u, d W+W+ u d Z0Z0 ν ν Z0Z0 e−e− e−e− Z0Z0 e−e− νeνe W+W+ Electromagnetic.
Lino MiramontiJune 9-14, 2003, Nara Japan 1st Yamada Symposium Neutrinos and Dark Matter in Nuclear Physics.
A screening facility for next generation low-background experiments Tom Shutt Laura Cadonati Princeton University.
LENS-CAL I. Barabanov, V. Gurentsov, V. Kornoukhov Institute for Nuclear Research, Moscow and R. S. Raghavan, Virginia Tech LONU-LENS Blacksburg, Oct 15,
Status of the BOREXINO experiment Hardy Simgen Max-Planck-Institut für Kernphysik / Heidelberg for the BOREXINO collaboration.
The Earth Matter Effect in the T2KK Experiment Ken-ichi Senda Grad. Univ. for Adv. Studies.
KamLAND : Studying Neutrinos from Reactor Atsuto Suzuki KamLAND Collaboration KEK : High Energy Accelerator Research Organization.
Using Reactor Anti-Neutrinos to Measure sin 2 2θ 13 Jonathan Link Columbia University Fermilab Long Range Planning Committee, Neutrino Session November.
Dec. 13, 2001Yoshihisa OBAYASHI, Neutrino and Anti-Neutrino Cross Sections and CP Phase Measurement Yoshihisa OBAYASHI (KEK-IPNS) NuInt01,
Present and future detectors for Geo-neutrinos: Borexino and LENA Applied Antineutrino Physics Workshop APC, Paris, Dec L. Oberauer, TU München.
Kr2Det: TWO - DETECTOR REACTOR NEUTRINO OSCILLATION EXPERIMENT AT KRASNOYARSK UNDERGROUND SITE L. Mikaelyan for KURCHATOV INSTITUTE NEUTRINO GROUP.
Monday, Feb. 19, 2007PHYS 5326, Spring 2007 Jae Yu 1 PHYS 5326 – Lecture #7 Monday, Feb. 19, 2007 Dr. Jae Yu 1.Neutrino Oscillation Experiments 2.Long.
1 MACRO constraints on violation of Lorentz invariance M. Cozzi Bologna University - INFN Neutrino Oscillation Workshop Conca Specchiulla (Otranto) September.
Latest Results from the MINOS Experiment Justin Evans, University College London for the MINOS Collaboration NOW th September 2008.
1 IDM2004 Edinburgh, 9 september 2004 Helenia Menghetti Bologna University and INFN Study of the muon-induced neutron background with the LVD detector.
Search for Electron Neutrino Appearance in MINOS Mhair Orchanian California Institute of Technology On behalf of the MINOS Collaboration DPF 2011 Meeting.
RENO & RENO-50 Soo-Bong Kim (KNRC, Seoul National University) “NOW 2014, Conca Specchiulla, Otranto, Lecce, Italy, September 7-14, 2014”
Data Processing for the Sudbury Neutrino Observatory Aksel Hallin Queen’s, October 2006.
Results from RENO Soo-Bong Kim (KNRC, Seoul National University) “17 th Lomosonov Conference on Elementary Particle Physics” Moscow. Russia, Aug ,
Determination of activity of 51 Cr source on gamma radiation measurements V.V.Gorbachev, V.N.Gavrin, T.V.Ibragimova, A.V.Kalikhov, Yu.M.Malyshkin,A.A.Shikhin.
Neutrino-­nucleus (nucleon) Reaction Measurement by J-PARC MLF sterile neutrino search experiment (J-PARC P56) Takasumi Maruyama (KEK) for J-PARC P56 working.
Search for Sterile Neutrino Oscillations with MiniBooNE
Daya Bay Reactor Neutrino Experiment On behalf of the DayaBay collaboration Virginia Polytechnic Institute and State University Joseph ykHor YuenKeung,
Medium baseline neutrino oscillation searches Andrew Bazarko, Princeton University Les Houches, 20 June 2001 LSND: MeVdecay at rest MeVdecay in flight.
1 Muon Veto System and Expected Backgrounds at Dayabay Hongshan (Kevin) Zhang, BNL DayaBay Collaboration DNP08, Oakland.
Recent Results from RENO NUFACT2014 August. 25 to 30, 2014, Glasgow, Scotland, U.K. Hyunkwan Seo on behalf of the RENO Collaboration Seoul National University.
Solar Neutrino Results from SNO
September 10, 2002M. Fechner1 Energy reconstruction in quasi elastic events unfolding physics and detector effects M. Fechner, Ecole Normale Supérieure.
Second Workshop on large TPC for low energy rare event detection, Paris, December 21 st, 2004.
5th June 2003, NuFact03 Kengo Nakamura1 Solar neutrino results, KamLAND & prospects Solar Neutrino History Solar.
Center for Neutrino Physics Source Neutrino Experiments Jonathan Link Center for Neutrino Physics Virginia Tech NuFact 2016.
Neutrino oscillations with radioactive sources and large detectors Wladyslaw H. Trzaska on behalf of: Yu.N. Novikov, T. Enqvist, A.N. Erykalov, F. v.Feilitzsch,
T2K Experiment Results & Prospects Alfons Weber University of Oxford & STFC/RAL For the T2K Collaboration.
Status and Prospects of Reactor Neutrino Experiments Soo-Bong Kim (KNRC, Seoul National University) “NuPhys 2014: Prospects in Neutrino Physics, London,
Double Chooz Experiment Status Jelena Maricic, Drexel University (for the Double Chooz Collaboration) September, 27 th, SNAC11.
Neutral Current Interactions in MINOS Alexandre Sousa, University of Oxford for the MINOS Collaboration Neutrino Events in MINOS Neutrino interactions.
IBD Detection Efficiencies and Uncertainties
Fast neutron flux measurement in CJPL
Neutrino Oscillations and T2K
SoLid: Recent Results and Future Prospects
Search for Sterile Neutrinos
Solar and Geo Neutrino Physics with Borexino RICAP
Donato Nicolo` Pisa University & INFN,Pisa
Simulation for DayaBay Detectors
Searches for Sterile neutrinos
Physics with the ICARUS T1800 detector
Sterile Neutrino Searches with Sources and Reactors
Signal and Background in LENS
KamLAND Update NuFact 05 Lauren Hsu June 21, 2005
Daya Bay Neutrino Experiment
Using Single Photons for WIMP Searches at the ILC
Toward realistic evaluation of the T2KK physics potential
Determination of Neutrino Mass Hierarchy at an Intermediate Baseline
Monoenergetic Neutrino Beam for Long Baseline Experiments
Davide Franco for the Borexino Collaboration Milano University & INFN
PBq 144Ce-144Pr source in KamLAND
Presentation transcript:

Search for sterile neutrinos with SOX: Monte Carlo studies of the experiment sensitivity Davide Basilico 1st year Workshop – 11/10/17 Tutors: Dott. Barbara Caccianiga, Prof. Emanuela Meroni

Outline Sterile neutrinos SOX project SOX analysis and sensitivity studies

Sterile neutrinos: experimental anomalies Neutrino flavor eigeinstates ≠ mass eigenstates → neutrino flavor oscillations Confirmed by several experiments ( ∆𝑚 21 2 =7.6⋅ 10 −5 eV 2 , ∆𝑚 31 2 =2.4⋅ 10 −3 eV 2 ); Anyway some experiments reveal «anomalies» : Accelerators : 𝜈 𝑒 appearance from 𝜈 𝜇 beam; Radiochemical: 𝜈 𝑒 events deficit (disappearance) from artificial sources Reactors: 𝜈 𝑒 events deficit (disappearance) short-baseline (L ∼ (10 − 100) m) Anomalies can not be included in the three-flavor model, since they hint towards a new mass squared difference ∆𝑚 𝑛𝑒𝑤 2 ~ eV 2

Sterile neutrinos Anomalies can be explained with a new neutrino state: It has to be sterile: interacts only through gravitational force (LEP constraints total number of active ν ) → impossible direct detection Indirect detection: active ν can oscillate in sterile states: New oscillation length justifies anomalies (oscillation parameters sin 2 2 𝜃 41 ≈0.11 , Δ 𝑚 41 ≈1.6 eV 2 ) Confirm/reject the sterile hypotesis with a new experiment: Search for sterile neutrinos with Borexino detector: SOX project

Borexino detector Scintillator sphere (300 ton) at LNGS, data-taking started in 2007 (mainly solar neutrinos) Extremely high shielding and radiopurity; 2200 PMTs collect scintillation photons: Energy → number of photons (σ E ∼ 3.5% @2 MeV); Position → photons time arrival (σ L ∼ 12 cm).

SOX project SOX goal: give a definitive answer to the sterile hypotesis. Measurements of 𝝂 𝒆 events coming from a flux of a powerful artificial source 𝜈 𝑒 source: 144Ce –144Pr , activity∼1.5 PBq, placed below Borexino Distance L ∼ m, energy E ∼ MeV Sensitive to ∆m2 ≈ E/L ∼ (0.1 − 10) eV2 Data taking in 2018 for 1.5 ys Detected through Inverse Beta Decay 𝜈 𝑒 +𝑝→𝑛+ 𝑒 + («golden channel») 8.5 m 𝝂 𝒆 source Expected events ∼ 10000 𝜈 𝑒 signal (source) ∼ 20-40 𝜈 𝑒 background (geo-neutrinos / reactors) → background-free experiment

Source transportation (Russia-Italy) SOX project Prompt (1.8-3 MeV): e+ annichilation → event L and E Delayed (2.2 MeV): γ emission after n capture e+ -n space/time/energy coincidence Energy threshold: 𝐸 𝑒 =1.8 MeV 144Ce-144Pr spectrum Source transportation (Russia-Italy)

WITH oscillation (example) ( sin 2 2 𝜃 41 =0.3 , Δ 𝑚 41 =2 eV 2 ) SOX – Analysis concept WITH oscillation (example) ( sin 2 2 𝜃 41 =0.3 , Δ 𝑚 41 =2 eV 2 ) NO oscillation Number of events as a function of distance from source (L) and energy (E) “Rate-only” analysis: total rate counting (search for 𝜈 𝑒 "disappearance" ) “Shape-only” analysis / oscillometry: events distribution as a function of L and E -> search for profile deformation due to the 𝜈 𝑒 → 𝜈 𝑠 oscillation

“Shape-only” analysis (blue) SOX Sensitivity Working on the SOX official sensitivity framework. Plot axis: sin 2 2 𝜃 41 , Δ 𝑚 41 2 Δm2< 0.2 eV2: osc.length longer than detector; 0.2 eV2 < Δ m2 < 1 eV2: entire oscilation length scanned: maximum sensitivity; Δ m2 > 1 eV2: osc.length smaller than resolution: “Rate-only analysis” Source activity Detection efficiency Active volume knowledge “Shape-only” analysis (blue) L ed E reconstruction Unmistakable sign for sterile oscillation existence

SOX Sensitivity Working on the SOX official sensitivity framework. Plot axis: sin 2 2 𝜃 41 , Δ 𝑚 41 2 Δm2< 0.2 eV2: osc.length longer than detector; 0.2 eV2 < Δ m2 < 1 eV2: entire oscilation length scanned: maximum sensitivity; Δ m2 > 1 eV2: osc.length smaller than resolution: Rate+Shape analysis (black): combined information from «rate only» and «shape only analysis»

SOX Sensitivity - Systematics Systematics related to the source Source activity uncertainty 144Ce-144Pr shape uncertainty Weakens knowledge on total expected events → rate analysis weakened Goal: σh=0.5% (red contour) Affects both rate and shape analysis Goal: σb=0.02 (red cont.)

New Borexino calibrations New detector calibrations (latest ones in 2009): Neutron detection efficiency Energy and position reconstruction Tuning Data-MC Radioactive sources (α, β, γ, n) in the scintillator through a rod system: Can be inclined and rotated System purification, ultrapure materials 2-3 months, beginning of 2018, 200 positions to be scanned

Summary SOX goal: conclusive answer to the sterile hypotesis; 𝜈 𝑒 MeV-energy intense source, events detected through IBD reaction; Sensitivity analysis rely on the total number events (“rate”) and on the events distribution (“shape”); Systematics: Source-related (uncertainty on the activity / 𝜈 𝑒 emitted spectrum); Detector-related (bias on position reconstruction -> to be studied carefully).

Thank you!

Borexino calibrations - Sources Neutrons (E<9 MeV): detector mapping for neutron detection efficiency α e β+: position reconstruction studies γ mono-energetic (E<3.2 MeV): energy response 2-3 months (2018) of intensive calibrations in 200 positions