KOTO実験による K中間子稀崩壊探索 南條 創 (京都大学)

Transcription

1 KOTO実験による K中間子稀崩壊探索 南條 創 (京都大学) 1

2 Contents Motivation KOTO Experiment Prospect 2

3 Motivation 3

4 New Physicsはあるのか 4

5 2008 : Kobayashi and Maskawa CP-violation was established. The size is not enough to explain matter dominant universe. New CP-violating particle is expected in higher energy scale : Englert and Higgs Higgs was discovered but it is far from closing the book. New physics in high energy scale is expected to stabilize Higgs mass. SUSY, little Higgs, Compositeness, Extra Dimension,? Dark matter? 5

6 New Physicsは存在する 物質優勢宇宙 Dark Matter... どうやって探す 6

7 New Physics Search High Energy Frontier High Intensity Frontier High energy frontier direct production of heavy particle High intensity frontier indirect access, high energy reach 一瞬の高エネルギースケール 稀なプロセス Multi-process approach 多方面からフレーバ構造を明らかに 標準理論の抑制 GIM, CKM,Helicity...suppression 精密な理論予測 Correlation is important. CP-violation is another guide. explanation of matter dominant universe 7

8 Why Kaon? Blanke '13 Generally most powerful GIM suppression of u and c quarks Hierarchical structure of CKM for t quark Most suppressed in s d transition (λ5) b d (λ3), b s (λ2) u c t d s 例えBs/d μμがsm-likeであっても s dはnpでエンハンス可能 b 8

9 Bona '07 Ishidori '13 Energy Reach Flavor structure MFV Generic Tree/Strong couple 5 TeV TeV Loop αs 0.5 TeV 2400 TeV Loop αw 0.2 TeV 800 TeV Tree/Strong couple ~1 Loop αs ~0.1 Loop αw ~0.03 (Bona '07) Genericの場合 K sectorが最強 104 TeVまでのリーチ なぜまだ見えない Energy scale, Flavor構造 Minimal Flavor Violation likeな場合 Bと強い相関 (NPでもCKMの構造を保持,新しいCPV phaseもない) 9

10 NP > 1 TeV? (ATLAS,CMS) Non-MFV like? (LHCb,CMS) Buras'13 10

11 Rare decay Strong suppression from CKM Buras '15 Small theoretical uncertainty ~2% High energy scale Hadron matrix element from tree process Ke3/Kmu3 Sensitive to new physics beyond the SM CP-violating process Related to charged mode Grossman-Nir bound : Model-independent inequality w/ iso-spin rotation 11

12 Status 10-8 Direct limit 2.6x10-8 (KEK E391a) 10-9 Indirect limit 1.5x10-9 (Grossman-Nir) New Physics? SM sensitivity 2.4x

13 SM extension w/ 4th generation ruled out Direct search EW precision test Higgs mass Otto '12 13

14 from ΔS=2とΔS=1のNPによる変化 同じnew phaseが支配 Z'/Z with Left / Right-handed coupling Littlest Higgs with T-parity 14

15 Input from ε'/ε Direct CPV from KL ππ Progress from lattice calculation Buras '15 SM expectation (Theory) Left and Right-handed coupling still can enhance Br(KL) MFV Left or Right-handed coupling 15

16 EW penguin contribute to e'/e in negative interference. Negative correlation btw Br(KL) Buras '15 16

17 Buras '15 Left- and right-handed coupling model can enhance Br(KL) 17

18 Buras '15 18

19 Littlest Higgs with T-Parity Blanke '15 Symmetry breaking scale 19

20 SUSY at TeV Tanimoto, Yamamoto '15 10 TeV SUSY still large enhancement on Br(KL) Less correlation btw Br(KL) and ε 50TeV SUSY still have enhancement factor on Br(KL) 20

21 Weekly-coupled light Z' with Lμ Lτ coupling Fuyuto '14 Explain g-2 with Mz'<400MeV also relate to B Kμμ from E949 experiment KOTO already access here. 21

22 KOTO Experiment 22

23 0 KOTO : K at TOkai Extraction J-PARC Accelerator High power Statistics of rare process Slow extraction Event pile-up due to high rate J-PARC 33kW (June 2015) ~ World-highest class 3GeV 30GeV 400MeV 23

24 Fixed Target Experiment High intensity proton beam+ Primary target High intensity secondary products Beam line Transport particles of interest Reduce unwanted particles Long life to transport. Gold 15mm x 6mm x 66mm 30 GeV proton 24

25 Particles mass and life time Bottom Strange Collider (τ D,B,t) Tools for fixed target experiment with high intensity proton driver Lower mass Longer life time Kaon has bee a special tool for fixed target experiment Pion Neutrino source Muon source 25

26 Kaon Low mass (0.5 GeV) Long life time (15m) Good for fixed target Strangeness Flavor Changing Neutral Current s d transition Flavor changing neutral current (GIM) Strong CKM suppression KL π0νν (Br 3x10-11 in SM) Direct CP-violation 26

27 Beam line 金標的 + proton KL beam line 電磁石 (charged) 20m長尺 (short-lived) コリメータ (beam halo) 細くシャープな中性ビーム(KL, γ, neutron) Pencil Beam 33kW 6sec cycle 4x10 proton 13 立体角 7.8μsr ~40%lost by decay ~107 KL 27

28 2nd collimator ( m) Beam plug 1st collimator 4m-long Dipole magnet 28

29 Signal Reconstruction 2γ+nothing Calorimeter + Beam constraint pencil beam Veto detectors 6.1m 29

30 Detector ~2m Veto : γ/charged reduction 30

31 History 100hours Detector upgrade 31

32 1st physics run in 2013 CKM2014 Sensitivity : 1.29x10-8 (Preliminary) ~ E391a sensitivity with only 100-hour run 1 event in the signal box 87 Number of observed data Well understood ± ±0.5 32

33 Main background source in E391a Halo neutron π0 at Upstream detector Downstream detector Largely reduced. E391a Final (5month) S.E.S : 1.11x10-8 KOTO 1st Physics run(4days) S.E.S : 1.29x ± ±0.5 33

34 Background source in KOTO ± ±0.5 CC05 CC06 Beam pipe 1m 34

35 Run in April-June 2015 Physics run 5.3 times higher POT run in May 2013 Calibration and special runs Calibration, Special runs Physics run in kW 29kW 26kW Physics 24kW 26kW X5.3 Integrated POT for May

36 0 Check with 3π sample Calorimeter and KL properties consistent with the run in May More detailed calibration is on-going Study to suppress background Black :April-May 2015 Red :May 2013 Area normalized Area normalized 36

37 To suppress halo neutron Upstream beam window Kapton 125um 12.5um Reduce neutron scattering Re-alined collimator Reduce neutron scattering on the collimator inner surface Hadron interaction events 37

38 Collimator alignment with new beam profle monitor Lead(1.5mm) Mirror Phosphor plate Re-alined collimators 38

39 To understand hadron interaction events Scattered at the target Core neutron 10 mm thick Al Contribution by Chonbuk Univ. * Removed in physics run Took Al-target data 70 hours > 15 times higher statics than May 2013 Hadron interaction Gammas from π0 Reconstructed PT (MeV/c) Reconstructed Z vertex (mm) 39 Developing BG reduction with cluster shape

40 To suppress low P T events CC05 CC06 Beam pipe Plastic scintillator WLS fiber 1m PMT Beam pipe (5mm t) SUS Aluminum Installed Beam Pipe Charged Veto Plastic scintillator 5-mm thick Wavelength shifting fber readout ~1/60 reduction expected 40

41 To suppress KL 2π0 Added modules X0: Photon punch-through inefficiency 1/5 In-beam photon veto Lead and Aerogel Cherenkov detector Lead and Acrylic Cherenkov detector 41

42 Prospect 42

43 0 To suppress KL 2π more Install inner barrel detector in winter 2015 Add 5 X0 to 13.5 X0 of current Main Barrel Suppress punch-through ineffciency by 1/50. Gluing fber to scintillator was mostly fnished. Module assembly will start soon. Will install it in this winter + Maintenance for existing broken channels in vacuum 43

44 Plan NA62 will take 100 events toward 2017 for Push Grossman-Nir limit down. We will overcome our background and improve our sensitivity 2015 April-June 2015 Fall

45 Long term plan 45

46 Summary New physics scenario MFV or non-mfv? Similar to MFV Z' model, generic SUSY,.. will still enhance Br(KL) largely NP in 5 TeV still enhance Br(KL) largely SM extension with 4 generation ruled out Littlest Higgs with T-parity under pressure from B μμ KOTO already have discovery potential for light Z' with ~π0 mass Sensitivity ~ current limit with only 100 hours data New background mechanism neutron Restarted in 2015 Non-MFV with left and right-handed coupling 1st Physics run in 2013 Br(KL π0νν) ε'/ε > SM? will suppress Br(KL) enhancement Strong correlation pattern from εk Non-MFV with only left or right-handed coupling MFV like KOTO already took 5.3 times larger statistics Data to study neutron background Calibration and study to suppress neutron background Prospects Will overcome neutron background Will search O(10-11) area for Br(KL) ~2018 Continue to KOTO Step2 in enlarged Hadron Experimental Facility 46