MEG. 2.1 KEK PSI PSI MEG II [4] GeV 2. Tevatron [5] 2017 ( 29 ) 12 12

Similar documents
LFV with µ-beams: status and perspectives

The MEG/MEGII and Mu3e experiments at PSI. Angela Papa Paul Scherrer Institut on behalf of the MEG/MEGII and Mu3e collaborations

clfv searches using DC muon beam at PSI

Status and Future of the PSI Experiment *

Final Results from the MEG Experiment and the Status of MEG-II

arxiv: v1 [physics.ins-det] 1 Sep 2009

Results and perspectives of the MEG and MEG II experiments

Lepton Flavour Violation

Experimental Searches for Muon to Electron Conversion

LIQUID XE DETECTOR FOR MU E GAMMA SEARCH

Update from the Mu3e Experiment

Lepton Flavor Violating Decays Review & Outlook

Liquid xenon gamma-ray calorimeter for the MEG experiment

MEG II 実験の準備状況と 今後の展望 東京大学 素粒子物理国際研究センター 岩本敏幸 他MEG II コラボレーション 2018年9月14日 日本物理学会2018年秋季大会 信州大学 JSPS Core-to-Core Program

The MEG experiment at PSI

PoS(TIPP2014)033. Upgrade of MEG Liquid Xenon Calorimeter. Ryu SAWADA. ICEPP, the University of Tokyo

arxiv: v4 [hep-ex] 2 Sep 2011

Kenji Ozone (ICEPP, Univ. of Tokyo, Japan) Outline. Introduction prototype R&D ー PMTs ー small & large type summary

The MEG Experiment at PSI: a sensitive search for

Charged Lepton Flavour Violation:

Mu2e: Coherent μ e Conversion Experiment at Fermilab. David Brown, LBNL representing the mu2e collaboration

COMET muon conversion experiment in J-PARC

LXe (part B) Giovanni Signorelli. Istituto Nazionale di Fisica Nucleare, Dipartimento di Fisica and Scuola Normale Superiore, Pisa (Italy)

Intense Slow Muon Physics

Fundamental Symmetries III Muons. R. Tribble Texas A&M University

The Mu2e Transport Solenoid

Overview of the COMET Phase-I experiment

CsI Calorimeter for KOTO experiment

The First Results of K2K long-baseline Neutrino Oscillation Experiment

MuSIC- RCNP at Osaka University

The PIENU Experiment a sensitive probe in the search for new physics

Muon Experiments. Masaharu Aoki, Osaka University. NP02 International workshop on Nuclear and Particle Physics at 50-GeV PS Kyoto

Data Analysis for the MEG Experiment. Francesco Renga & Cecilia Voena INFN Roma

MEG Lepton Flavor Violation Search:

Lepton Flavor Violation Experimental Overview

arxiv: v1 [physics.ins-det] 26 Sep 2018

A survey of the rare pion and muon decays.

Neutron Structure Functions and a Radial Time Projection Chamber

The Mu3e PSI

The doubly charged scalar:

LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration

PoS(ICHEP2016)552. The Mu3e Experiment at PSI. Alessandro Bravar University of Geneva

The Mu3e PSI

The first muon beam from a new high-intensity DC muon source, MuSIC

PSI. Muon Experiment at the PSI, KEK

The W-mass Measurement at CDF

The Neutrino of the OPERA:

Measurements of the W Boson Mass and Trilinear Gauge Boson Couplings at the Tevatron

Proposal to measure the muon electric dipole moment with a compact storage ring at PSI

Recent Results from K2K. Masashi Yokoyama (Kyoto U.) For K2K collaboration 2004 SLAC Summer Institute

Measurements of liquid xenon s response to low-energy particle interactions

Abstract. To be published in the Proceedings of the 8th International Workshop On Tau Lepton Physics September 2004, Nara, Japan

Search for a Dark Photon: proposal for the experiment at VEPP 3.

CPT ALPHA CPT 2.1 CPT , CERN. TRIUMF Canada s National Laboratory for Particle and Nuclear Physics

The Mu3e Experiment. Niklaus Berger. Physics Institute, University of Heidelberg. Charged Lepton Flavour Violation Workshop, Lecce, May 2013

Beam at the Paul Scherrer Institut

Waseda University. Design of High Brightness Laser-Compton Light Source for EUV Lithography Research in Shorter Wavelength Region

arxiv: v1 [hep-ex] 7 Sep 2016

Recent results at the -meson region from the CMD-3 detector at the VEPP-2000 collider

The MUon proton Scattering Experiment (MUSE) at the Paul Scherrer Institute

New Limits on Heavy Neutrino from NA62

Higgs Searches and Properties Measurement with ATLAS. Haijun Yang (on behalf of the ATLAS) Shanghai Jiao Tong University

An Experimental Proposal on Nuclear and Particle Physics Experiments at the J-PARC 50 GeV Proton Synchrotron

17/01/17 F. Ould-Saada

ATHENA / AD-1. First production and detection of cold antihydrogen atoms. ATHENA Collaboration. Rolf Landua CERN

Final results from K2K and status of T2K

HQL Virginia Tech. Bob Hirosky for the D0 Collaboration. Bob Hirosky, UNIVERSITY of VIRGINIA. 26May, 2016

Neutrino Factory in Japan: based on FFAG

Search for pentaquark Θ + in hadronic reaction at J-PARC. M. Naruki for the E19 collaboration 2012/8/24 FB20, Fukuoka

PoS(FPCP2009)057. Chloé Malbrunot (for the PIENU collaboration ) University of British Columbia Vancouver, Canada

Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders

FERMI NATIONAL ACCELERATOR LABORATORY

PHYS 3446 Lecture #15

PoS(NOW2016)003. T2K oscillation results. Lorenzo Magaletti. INFN Sezione di Bari

Particle Physics with Electronic Detectors

Neutrino oscillation physics potential of Hyper-Kamiokande

PoS(EPS-HEP2011)250. Search for Higgs to WW (lνlν, lνqq) with the ATLAS Detector. Jonas Strandberg

LHCb: Reoptimized Detector & Tracking Performance

Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France.

Polarized muon decay asymmetry measurement: status and challenges

Hadron Physics at LEPS2

Oliver Stelzer-Chilton University of Oxford High Energy Physics Seminar Michigan State University

Belle Hot Topics. Nagoya University Koji Ikado (for the Belle Collaboration) Flavor Physics and CP Violation Conference (FPCP2006) Apr.

Measurement of Properties of Electroweak Bosons with the DØ Detector

Track reconstruction for the Mu3e experiment Alexandr Kozlinskiy (Mainz, KPH) for the Mu3e collaboration DPG Würzburg (.03.22, T85.

HIEPA2018, Beijing March 19-21, Two-photon Physics. Simon Eidelman

Error Budget in π + e + ν Experiment

PoS(EPS-HEP2017)238. Experimental limiting factors for the next generation

Introduction to the Neutrino Factory

Accelerators and Colliders

D 0 -D 0 mixing and CP violation at LHC

Review of LHCb results on MPI, soft QCD and diffraction

Why do we accelerate particles?

Latest Results from the OPERA Experiment (and new Charge Reconstruction)

Search for heavy neutrinos in kaon decays

η and η physics at BESIII

Precise measurements of the W mass at the Tevatron and indirect constraints on the Higgs mass. Rencontres de Moriond QCD and High Energy Interactions

Measurement of the neutrino velocity with the OPERA detector in the CNGS beam

Masaharu Aoki Osaka University

PoS(TIPP2014)093. Performance study of the TOP counter with the 2 GeV/c positron beam at LEPS. K. Matsuoka, For the Belle II PID group

Transcription:

27 MEG µ + e + γ mori@icepp.s.u-tokyo.ac.jp 27 ( 29 ) 2 2 MEG Mu-E-Gamma [] 999 KEK PSI [2] PSI PSI 6 7 27 28 23 µ eγ 26 4.2 3 [3] MEG II [4] MEG 2 µ eγ µ eγ a µ eγ 54 µ eγ b µ eγ : a b µ eγ 2. 99 CERN LEP Z 6 GeV 2 995 LEP 75 GeV Tevatron µ eγ 4 [5] µ eγ

2 28 µ eγ µ eγ [6] µ eγ [7] 996 PSI 997 µ eγ PSI 998 Letter of Intent [8] 999 [2] µ eγ O( 2 ) 22 LHC 25 GeV LHC 25 b LHC LHC µ eγ LHC 3: a µ µ eγ [] 2: LEP 6 GeV a µ = (29 ± 8) µ eγ 2 δ 2 LL = 4 3 µ 3e µn en µ eγ 2.2 LHC b a µ =(g µ 2)/2 26 a µ [9] 3.5σ µ eγ 3 a µ a µ B(µ eγ) [] µ + e + e e + µ 3e µ N e N N µ eγ α / B(µ + e + e e + ).6 B(µ + e + γ) R(µ Al e Al).26 B(µ + e + γ) R(µ N e N)

3 29 µ 3e µn en µ eγ 4 MEG µ 3e µn en 22 O( 4 ) µ eγ µ eγ µ 3e µn en µ eγ µ 3e µn en 4: µ eγ 9% µ 3e µn en µ eγ MEG II COMET-II/Mu2e Mu3e-III 4 µ eγ µ eγ 52.8 MeV 28-29 MeV/c % µ eγ µ eγ 3 3 % 7 µ + e + ν ν µ eγ AIF: Annihilation in Flight µ eν νγ µ eγ 52.8 MeV % 5% 4 µ eγ 52.8 MeV

4 3 7 52.8 MeV MEG [] 5 5. PSI 7 8 PSI PSI 59 MeV 2.2-2.4 ma.4 MW 5.6 MHz RF 2 µsec PSI 3. ma.8 MW 4 cm MEG πe5 66 BTS COBRA BTS COBRA 2.3 cmφ 25 µm 2 Rohacell 5 6 3 7 /sec 2 3 5: MEG µ eγ 5 MEG µ eγ 7 8 5.2 COBRA 3 7 COBRA COnstant Bending RAdius 3 5 5 7.27 T.49 T 7 a COBRA

5 3 μ + e + (a) 6: COBRA 6 7 b COBRA COBRA.2X µ eγ 52.8 MeV 85% KEK COBRA COBRA 5 µsr 45 MeV/c DC DC TC 5 DC TC μ + e + (b) 7: COBRA a b DC 52.8 MeV AIF COBRA DC 6 6 9 7 mm 2 2 COBRA khz Charge Division DC 2.5 µm 25 nm DC.5 Pa 52.8 MeV 2 3 X 52.8 MeV.58% σ 8

6 32 Number of events /(.25 MeV) Relative efficiency 5 5.5 4 45 5 55 E e (MeV) 8: Number of events /(.8 nsec) 8 6 4 2 N RMD = 37 ± 42 sigma = 23 ± 3 ps -2-2 (nsec) 9: t eγ 5.3 t eγ DC TC TC 5 4 4 9 cm 3 TC COBRA cm TC TC TC DC TC 5 7 ps DC TC ps TC 9 22 ps Z 2 : 2 846 MEG

7 33 2.8 cm NaI 75 % 45 nsec 8 l 846 2 Radiative decay & e + annihilation Number of events /(.5 MeV) 5 2 (a) (b) w < 2 cm w > 2 cm Pileup Cosmic ray 2: 3 4 5 6 7 (MeV) : 54.9 MeV a 2 cm b 2 cm 5 mm 5 MeV 65 7 psec E γ KEK COBRA C [2] µ eγ DRS: Domino Ring Sampler DRS

8 34 Energy scale (arb. unit) Xe 2 ppb 3m 2/7 29 2 2 22 23.4.2.98 Timing Counter target LXe Detector Drift Chamber Muon Beam 4:.96 3/2 /9 / /7 3/8 3/ 3/8 3/ 3/2 2/7 29 2 2 22 23 3:.2% rms 7.6 MeV 2 π p π n 8 54.9 MeV 82.9 MeV 54.9 MeV 52.8 MeV 54.9 MeV µ eγ b a.7 2.4% CW COBRA 7.6 MeV 3-4 CW 2 7.6 MeV 3.2% rms 24 Am 9 MeV 6 µ + e + γ MEG 28 [3] 4 [3, 4] 29 [5] µ eγ Likelihood PDF

9 35 E γ (MeV) 58 56 54 52 t eγ (nsec) 2.5.5.5 events / 56 (ps) 45 (a) 4 35 3 25 2 5 events /.24 (MeV) 8 7 6 5 4 3 2 (b) events /.4 (MeV) 3 2 (c) 5.5 5.6.4.2.2.4.6 (ns) t e + γ E e + 5 5 52 53 54 55 56 (MeV) 48 5 52 54 56 58 E γ (MeV) 48 5 5 52 53 54 55 56 E e (MeV) 2.9995.999.9985 cosθ eγ 5: MEG µ eγ σ.64σ 2σ t eγ cos Θ eγ 9% cos Θ eγ <.99963 t eγ <.24 ns E γ 7% E e 9% 5. < E γ < 55.5 MeV 52.4 <E e < 55. MeV Θ eγ PDF 48 <E γ < 58 MeV t eγ < ns µ eγ Likelihood 4 5 MEG E γ, E e, t eγ, cos Θ eγ σ events / 2. (mrad) 4 35 3 25 2 5 5 4 2 2 4 (mrad) e + γ (d) events / 3. (mrad) 4 (e) 35 3 25 2 5 5 6 4 2 2 4 6 (mrad) e + γ events /.6 3 (f) 2 8 6 4 2 2 4 R sig 6: a e Likelihood MEG f R sig 9% Likelihood 6 a e Likelihood 6 f R sig log (S/(f R R + f A A)) S R A PDF f R f A 29-2 22-23 -.3-5.5-2.2 9% CL 6. 7.9 4.2 8. 8.2 5.3 : µ eγ 3 9% C.L. Profile Likelihood Ratio Frequentist Approach 9% µ eγ µ eγ 3.5%

36 28 3 MEG µ eγ 4.2 3 9% C.L. MEG 3 7 3 3 ILC K CP 3 B µ eγ MEG II KEK MEG MEG 224 264 [] http://meg.icepp.s.u-tokyo.ac.jp/. [2] T. Mori et al., Research Proposal to PSI, R- 99.5., May 999. [3] A.M. Baldini et al. (MEG Collaboration), Eur. Phys. J. C, 76:434, -3 (26). [4] A.M. Baldini et al. (MEG II Collaboration), arxiv:3.7225 (23); MEG II Design Report. [5] R. Barbieri and L.J. Hall, Phys. Lett. B338 (994) 22; R. Barbieri, L.J. Hall, and A. Strumia, Nucl. Phys. B445 (995) 29. [6] J. Hisano and D. Nomura, Phys. Rev. D 59 (999) 65. [7] 2,, UT-ICEPP 96-2, April 996. [8] A.v.d.Schaaf et al., Letter of Intent for an experiment at PSI, R-98-5., May 998. LoI [9] G.W. Bennett et al., Phys. Rev. D 73 (26) 723. [] G. Isidori, F. Mesia, P. Paradisi, D. Temes, Phys. Rev. D 75 (27) 59. [] J. Adams et al. (MEG Collaboration), Eur. Phys. J. C, 73, 2365 (23). [2], 26-, 9 (27). [3], 28-4, 227 (2). [4] J. Adams et al. (MEG Collaboration), Nucl. Phys. B 834, -2 (2); Phys. Rev. Lett. 7, 78 (2); Phys. Rev. Lett., 28 (23). [5],, 29-3, 33 (2); R. Sawada, Proceedings of ICHEP2, Paris, France, PoS (ICHEP 2) 263. 2 PRL [4]