Correlated Background measurement in Double Chooz experiment

Similar documents
Daya Bay and joint reactor neutrino analysis

Neutrinos. Why measure them? Why are they difficult to observe?

Double Chooz Sensitivity Analysis: Impact of the Reactor Model Uncertainty on Measurement of Sin 2 (2θ 13 )

The Daya Bay Reactor Neutrino Oscillation Experiment

Particle Physics: Neutrinos part I

Status of 13 measurement in reactor experiments

The Search for θ13 : First Results from Double Chooz. Jaime Dawson, APC

arxiv: v1 [hep-ex] 14 May 2015

Daya Bay Neutrino Experiment

Observation of Reactor Antineutrinos at RENO. Soo-Bong Kim for the RENO Collaboration KNRC, Seoul National University March 29, 2012

Neutrino Experiments with Reactors

Measurement of q 13 in Neutrino Oscillation Experiments. Stefan Roth, RWTH Aachen Seminar, DESY, 21 st /22 nd January 2014

Precise measurement of reactor antineutrino oscillations at Daya Bay

arxiv:hep-ex/ v1 15 Aug 2006

Latest Results of Double Chooz. Stefan Schoppmann for the Double Chooz Collaboration

The Daya Bay Reactor Neutrino Experiment

New results from RENO and prospects with RENO-50

Steve Biller, Oxford

The Double Chooz Project

章飞虹 ZHANG FeiHong INTERNATIONAL SCHOOL OF SUBNUCLEAR PHYSICS Ph.D. student from Institute of High Energy Physics, Beijing

Jelena Maricic Drexel University. For Double Chooz Collaboration. Spain. France. Germany U.S.A. Japan Russia. Brazil U.K. Courtesy of T.

New Results from RENO

An Underground Laboratory for a Multi-Detector Experiment. Karsten Heeger Lawrence Berkeley National Laboratory

PoS(NEUTEL2017)007. Results from RENO. Soo-Bong Kim. for the RENO collaboration Seoul National University, Republic of Korea

The Daya Bay Reactor Neutrino Experiment

Status of The Daya Bay Reactor Neutrino Experiment

The Double Chooz reactor neutrino experiment

The ultimate measurement?

Recent Results from RENO & Future Project RENO-50

The Double Chooz experiment

Double Chooz and non Asian efforts towards θ 13 Journal of Physics: Conference Series

Neutrino Physics. Neutron Detector in the Aberdeen Tunnel Underground Laboratory. The Daya Bay Experiment. Significance of θ 13

Daya Bay Neutrino Experiment NUFACT05. Jun Cao. Institute of High Energy Physics, Beijing

The Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos

arxiv: v1 [hep-ex] 11 May 2017

arxiv: v1 [hep-ex] 4 Mar 2014

NEW νe Appearance Results from the. T2K Experiment. Matthew Malek Imperial College London. University of Birmingham HEP Seminar 13 June 2012

Sterile Neutrino Experiments at Accelerator

PoS(HQL2014)018. Reactor Antineutrino Experiments Double Chooz and RENO

Neutrino Masses and Mixing

Neutrino Experiments with Reactors

Observation of Mixing Angle 13

Recent oscillation analysis results from Daya Bay

Recent T2K results on CP violation in the lepton sector

Wei Wang University of Wisconsin-Madison. NNN09, Estes Park, Colorado, Oct 8, 2009

저작권법에따른이용자의권리는위의내용에의하여영향을받지않습니다.

Short baseline neutrino oscillation experiments at nuclear reactors

KamLAND. Studying Neutrinos from Reactor

Neutrino Experiment. Wei Wang NEPPSR09, Aug 14, 2009

Current Results from Reactor Neutrino Experiments

Neutrino Experiments: Lecture 3 M. Shaevitz Columbia University

The Daya Bay Anti-neutrino Experiment

arxiv: v1 [hep-ex] 1 Dec 2015

Reactor Neutrino Oscillation Experiments: Status and Prospects

KamLAND. Introduction Data Analysis First Results Implications Future

Status and Prospects of Reactor Neutrino Experiments

Solar spectrum. Nuclear burning in the sun produce Heat, Luminosity and Neutrinos. pp neutrinos < 0.4 MeV

Latest results from Daya Bay

Neutrino Experiments: Lecture 2 M. Shaevitz Columbia University

Results on geoneutrinos at Borexino experiment. Heavy Quarks and Leptons Yamagata Davide Basilico

Reactor-based Neutrino Experiment

Bari Osmanov, University of Florida. OscSNS - proposal for neutrino experiment at ORNL SNS facility

Neutron background and possibility for shallow experiments

New Results for ν µ ν e oscillations in MINOS

PoS(ICHEP2016)474. SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor

arxiv: v4 [physics.ins-det] 27 Nov 2014

RENO & RENO-50. RENO Reactor Neutrino Experiment. RENO = Reactor Experiment for Neutrino Oscillation. (On behalf of RENO Collaboration)

Andrey Formozov The University of Milan INFN Milan

- Future Prospects in Oscillation Physics -

50 years of Friendship Mikhail Danilov, LPI(Moscow)

Observation of Reactor Electron Antineutrino Disappearance & Future Prospect

PHYS 5326 Lecture #2. Wednesday, Jan. 24, 2007 Dr. Jae Yu. Wednesday, Jan. 24, 2007 PHYS 5326, Spring 2007 Jae Yu

Chart of Elementary Particles

Observation of Reactor Antineutrino Disappearance at RENO

Prospects for Measuring the Reactor Neutrino Flux and Spectrum

Precise sin 2 2θ 13 measurement by the Daya Bay reactor neutrino experiment.

Search for Sterile Neutrinos with the Borexino Detector

Particle Physics. Michaelmas Term 2009 Prof Mark Thomson. Handout 11 : Neutrino Oscillations. Neutrino Experiments

Neutrino mixing II. Can ν e ν µ ν τ? If this happens:

Search for Oscillation with Lithium-6 Detector at BR2 Prototype Update and short perspectives

Recent Discoveries in Neutrino Physics

A Large Liquid Scintillator Detector for Neutrino Mass Hierarchy : RENO-50

Reactor On/Off Monitoring with a Prototype of Plastic Anti-neutrino Detector Array (PANDA)

Search for sterile neutrinos at the DANSS experiment

reactor θ13 the ultimate measurement?) Anatael Cabrera LIO Lyon (France) October 2012 CNRS / IN2P3 Double APC (Paris)

A Trial of Neutrino Detection from Joyo Fast Research Reactor

Available online at ScienceDirect. Physics Procedia 61 (2015 ) K. Okumura

NEUTRINO OSCILLATION EXPERIMENTS AT NUCLEAR REACTORS

New Results from the MINOS Experiment

Searches for sterile neutrinos at the DANSS experiment. Dmitry Svirida for the DANSS Collaboration ITEP-JINR

θ13 Measurements with Reactor Antineutrinos

Oak Ridge and Neutrinos eharmony forms another perfect couple

Observation of Electron Antineutrino Disappearance at Daya Bay

Particle Physics WS 2012/13 ( )

Oscillating Neutrinos and T2K

Measuring the neutrino mass hierarchy with atmospheric neutrinos in IceCube(-Gen2)

Recent results from Super-Kamiokande

Muons in Borexino. SFB Block Meeting. Daniel Bick Universität Hamburg. D. Bick (Uni HH) Muons in Borexino

Neutrino oscillation physics potential of Hyper-Kamiokande

Potential of Hyper-Kamiokande at some non-accelerator Physics and Nucleon Decay Searches

Transcription:

Correlated Background measurement in Double Chooz experiment Guillaume Pronost (Supervisor : Frederic Yermia) SUBATECH Journe es de Rencontres des Jeunes Chercheurs 2013

OUTLINE 1 - Neutrino Physics 2 - Double Chooz 3 - Correlated Background Measurement Journées de Rencontres des Jeunes Chercheurs 2013 2/24 gpronost@in2p3.fr

Neutrino Physics Neutrino Physics Journées de Rencontres des Jeunes Chercheurs 2013 3/24 gpronost@in2p3.fr

Neutrino Physics (Reminder) 3 neutrinos flavor described in Standard Model. One major property : Oscillations. A neutrino generated in a specific flavor can later be measured as another flavor. Described by the PMNS matrix (Pontecorvo, Maki, Nakagawa & Sakata) : U = 1 0 0 0 cos θ 23 sin θ 23 0 sin θ 23 cos θ 23 cos θ 13 0 sin θ 13.e iδ 0 1 0 sin θ 13.e +iδ 0 cos θ 13 cos θ 12 sin θ 12 0 sin θ 12 cos θ 12 0 0 0 1 θ 23 : P(ν µ ν µ ) by Atoms. ν and ν beam θ 13 : P(ν e ν e ) by Reactor ν θ 13 & δ : P(ν µ ν e ) by ν beam θ 12 : P(ν e ν e ) by Reactor ν and Solar ν 3 mixing angles : θ 23, θ 13 & θ 12. 2 mass difference scales : m 2 12 & m2 23 1 phase δ : CP violation in ν-sector Until November 2011 : only one upper limit for θ 13 Goal of Double Chooz : measure θ 13 Journées de Rencontres des Jeunes Chercheurs 2013 4/24 gpronost@in2p3.fr

Double Chooz Double Chooz Journées de Rencontres des Jeunes Chercheurs 2013 5/24 gpronost@in2p3.fr

Double Chooz site Near Detector At 400m Far Detector At 1050m Nuclear Core : 1021 ν e/s I International collaboration (Brazil, France, Germany, Japan, Russia, Spain, USA) I Site at Chooz (Ardennes, France) near Chooz Nuclear Plant. Journe es de Rencontres des Jeunes Chercheurs 2013 6/24 gpronost@in2p3.fr

Double Chooz experiment Measure of an ν e disappearance. Two identical detectors of 8.3 t ( Double Chooz) : Near detector. Measures the ν e flux before oscillations. Far detector. Measures the ν e flux after oscillations. Comparisons between expected and observed ν e flux allow to access to θ 13 measurement. Two phases in Double Chooz : First phase : Only Far detector. Non-oscillated flux provided by reactor core simulations. Second phase (half 2014) : Both detectors. Journées de Rencontres des Jeunes Chercheurs 2013 7/24 gpronost@in2p3.fr

Double Chooz detection principle : Inverse Beta Decay Inverse Beta Decay (IBD) : ν e + p e + + n e + (positron) quickly annihilates : Prompt Signal Visible energy = e + energy + annihilation γ s 1 12 MeV n (neutron) captured on Gd or H : Delayed Signal Visible energy = γ s from neutron capture on Gd / H 8 MeV or 2.2 MeV. Time interval : t 30µs In this talk : Only Gd selection. Journées de Rencontres des Jeunes Chercheurs 2013 8/24 gpronost@in2p3.fr

Double Chooz detector Outer Veto (OV) : Plastic Scintillator Used to cosmic µ detection Steel shield (15cm thick) Inner Detector (ID) ν-target : Gd loaded Liquid Scintillator Target of neutrino interaction (IBD) γ-catcher : Liquid Scintillator Measure γ escaped from ν-target Buffer : Mineral oil & 390 PMTs Reduction of γ from PMTs and from radioactivity. Steel tank (3mm) Inner Veto (IV) : Liquid Scintillator & 78 PMTs Used to cosmic µ and fast neutron detection Journées de Rencontres des Jeunes Chercheurs 2013 9/24 gpronost@in2p3.fr

Double Chooz detection : Backgrounds (Gd selection) Accidentals 9 Li Detector n.c. n µ Detector n.c. n 9 Li µ γ e n.c. : neutron capture Prompt signal : γ from radioactivity. Delayed signal : Fast Neutron from muon spallation in rock. Rate : 0.261 ± 0.002 events/day [1]. 9 Li e + n + 8 Be (τ 200 ms) Prompt signal : e. Delayed signal : neutron. Residual rate : 1.25 ± 0.54 events/day [1]. Journées de Rencontres des Jeunes Chercheurs 2013 10/24 gpronost@in2p3.fr

Double Chooz detection : Correlated Background (Gd selection) Fast Neutrons Stopping Muon Detector p.r. n µ Detector µ n.c. n e p.r. : proton recoil n.c. : neutron capture Prompt signal : γ from radioactivity. Delayed signal : Fast Neutron from muon spallation in rock. Rate : 0.30 ± 0.14 events/day [1]. µ e + ν e + ν µ (τ 2 µs) Prompt signal : short µ track. Delayed signal : Michel e (from µ decay) Rate : 0.34 ± 0.18 events/day [1]. Journées de Rencontres des Jeunes Chercheurs 2013 11/24 gpronost@in2p3.fr

Correlated Background Measurement Correlated Background Measurement Journées de Rencontres des Jeunes Chercheurs 2013 12/24 gpronost@in2p3.fr

Problematic of a Correlated Background Measurement Prompt energy spectrum [2] Estimation of Correlated Backgroud : Extend E prompt cut up to 30 MeV. Between 12 MeV < E prompt < 30 MeV, no IBD expected Correlated Background. Journées de Rencontres des Jeunes Chercheurs 2013 13/24 gpronost@in2p3.fr

Problematic of a Correlated Background Measurement Prompt energy spectrum [2] Estimation of Correlated Backgroud at Low Energy : Daya Bay, RENO : Flat shape assumption. Double Chooz : Direct measurement (in this talk : Inner Veto Tagging method) Journées de Rencontres des Jeunes Chercheurs 2013 14/24 gpronost@in2p3.fr

Why Inner Veto Tagging? Correlated Background : Events from outside detector. Fast Neutron (FN) : Lot of FN generated by µ some expected to hit Inner Veto (IVTagged). Stopping Muon (SM) : from cheminey few expected to hit Inner Veto. Select a pur sample of IVTagged Fast Neutron should give the shape of FN at low energy. SM µ FN µ IV ID n IV ID n.c. p.r. : proton recoil n.c. : neutron capture p.r. e p.r. 0 However : Other kind of events can be IVTagged. Journées de Rencontres des Jeunes Chercheurs 2013 15/24 gpronost@in2p3.fr

Fast Neutron / Stopping Muon separation Time correlation between prompt and delayed events [2] τ (µ) 2µs : Separation between Fast Neutron and Stopping Muon done by using t[prompt Delayed] In this talk : Only Fast Neutron shape estimation. Journées de Rencontres des Jeunes Chercheurs 2013 16/24 gpronost@in2p3.fr

IVTagged events IVTagged events : γ/n + ν e ν e FN µ γ γ n IV ID IBD n IV p.r. ID p.r. n.c. IV ID n.c. γ γ/n γ p.r. : proton recoil n.c. : neutron capture How to separate these events? Use correlations : ID Time ID Space ID-IV Time ID-IV Space Fast Neutron Some Some Some Some γ/n (IV) + ν e (ID) Some Some None None γ-γ + n/γ None None Strong Strong Journées de Rencontres des Jeunes Chercheurs 2013 17/24 gpronost@in2p3.fr

Space Correlation between Prompt and Delayed : γ γ rejection Space correlation between Prompt and Delayed γ γ : Come from accidental background. Prompt-Delayed space correlation up to 1500 mm. Cut on R(Prompt Delayed) < 1500 mm Reduction to 2% of remaining IVT sample. Journées de Rencontres des Jeunes Chercheurs 2013 18/24 gpronost@in2p3.fr

Time Correlation between ID and IV : ν e rejection Time correlation between ID and IV versus Prompt energy Untagged sample IVTagged Sample [2] ID-IV Time correlation between [ 2, 95] ns. Cut on t(id IV) [ 2, 95] ns Reduction to 12% of remaining IVT sample. Journées de Rencontres des Jeunes Chercheurs 2013 19/24 gpronost@in2p3.fr

Fast Neutron shape with IVT method In last DC publication : Purity of Fast Neutron sample : 86% Non-flat shape for Fast Neutron. Yet, big uncertainties. [2] Journées de Rencontres des Jeunes Chercheurs 2013 20/24 gpronost@in2p3.fr

(Preliminary) Space correlation between ID and IV Since last publication : development of an algorithm to reconstruct position in IV. We can use space correlation between IV and ID to improve Fast Neutron sample purity. Space Correlation between ID and IV 14 After ID Space & ID-IV Time cuts 12 Buffer GC Rejected by ID-IV Time cut Rejected by ID Space cut 10 γ γ contamination 8 6 Preliminary ν e contamination 4 2 0 0 1 2 3 4 5 6 (m) Distance Veto-Prompt Journées de Rencontres des Jeunes Chercheurs 2013 21/24 gpronost@in2p3.fr

Summary Double Chooz : Experiment to measure θ 13 value. Detection of Inverse Beta Decay in detectors. Three main background : Accidentals, 9 Li and Correlated. Correlated background : Fast Neutron from cosmic muon spallation in rocks. Stopping Muon decay in detector Target. Shape at Low Energy : Flat assumption is most part of other reactor experiment. Direct measure in Double Chooz. Inner Veto Tagging : Method to measure the low energy shape for Fast Neutron. Different kind of events tagged. Separation with correlation in ID or between ID and IV. [Preliminary] Space correlation add in the method to improve purity. Journées de Rencontres des Jeunes Chercheurs 2013 22/24 gpronost@in2p3.fr

References [1] : K. Abe et al. (Double Chooz Collaboration), Reactor ν e disappearance in the Double Chooz experiment, Phys. Rev. D 86, 052008 (2012) [2] : A. Remoto thesis Journées de Rencontres des Jeunes Chercheurs 2013 23/24 gpronost@in2p3.fr

Correlated Background Energy spectrum Correlated Background Energy spectrum Journées de Rencontres des Jeunes Chercheurs 2013 24/24 gpronost@in2p3.fr