The 3rd Tohoku University GCOE International Symposium

Similar documents
: status and prospects

What is different at Belle II?

First light from. Gagan Mohanty

Belle/Belle II CsI(T l ) electromagnetic calorimeter

Impact of the Belle II Pixel Detector on CP-Violation Measurements

Lepton Number and Universality Violation at Belle

Super KEKB and Belle II: Status of the KEK Super B Factory

The Making of the Belle II Experiment

Impact of the PXD on the Vertex Reconstruction of π 0 particles

Recent Results on the Measurement of Fragmentation Functions in e + e - Annihilation

Belle II status and prospects for flavor physics. Jing-Ge Shiu/NTU On behalf of the Belle II collaboration

Belle II perspectives on Unitarity Triangle sides and angles

NEXT GENERATION B-FACTORIES

Status and Future Prospects for Charged Lepton Flavor Violation Searches at B Factories and Belle-II

Study of charmoniumlike states with initial state radiation at Belle II

Sensitivity Study for B 0 π 0 π 0

DEPFET sensors development for the Pixel Detector of BELLE II

Brief Report from the Tevatron. 1 Introduction. Manfred Paulini Lawrence Berkeley National Laboratory Berkeley, California 94720

Future Belle II experiment at the KEK laboratory

Recent XYZ results from Belle

PoS(HQL 2012)021. The LHCb upgrade. Tomasz Szumlak 1

CP Violation sensitivity at the Belle II Experiment

Status of the LHCb Experiment. Ueli Strauman, University of Zurich, Switzerland. Sept. 13, 2001

LHC status and upgrade plan (physics & detector) 17 3/30 Yosuke Takubo (KEK)

CP Violation and Rare B Decays at Belle

Results of same sign dilepton charge asymmetry from Belle and BaBar

Observation of Large CP Violation in the Neutral B Meson System

CKM fits at SuperKEKB

b Physics Prospects For The LHCb Experiment Thomas Ruf for the LHCb Collaboration Introduction Detector Status Physics Program

Flavor Physics beyond the SM. FCNC Processes in the SM

B-Physics Potential of ATLAS, CMS, LHCb and BTeV

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

SuperKEKB and Belle II Status Report

THE PEP-II B-FACTORY AND THE BABAR DETECTOR

The LHCb Upgrade. On behalf of the LHCb Collaboration. Tomasz Szumlak AGH-UST

Status of PEP-II and BaBar. 1 Introduction. 2 PEP-II Machine

Next Generation B-factories

SUSY-related Lepton and Hadron Flavor Results from Belle Yutaro Sato

Tests of the BURLE 64-anode MCP PMT as the detector of Cherenkov photons

News from the KEK Meetings

a) National Laboratory for High Energy Physics (KEK), b) Saga University, c) National Kaohsiung Normal University, d) National Taiwan University,

Construction Status of SuperKEKB

New Physics search in penguin B-decays

Inclusive B decays with mesons and other flavor puzzles at Belle and Belle II

Peter Križan. University of Ljubljana and J. Stefan Institute. ECFA Plenary Meeting, CERN, Nov 25-26, University of Ljubljana

Heavy flavor meson(-like) spectroscopy at Belle/Belle II. Kenkichi Miyabayashi Nara Women s at Tokai 2015 Aug.

Hadronic vs e + e - colliders

e + e Factories M. Sullivan Presented at the Particle Accelerator Conference June 25-29, 2007 in Albuquerque, New Mexico e+e- Factories

D Hadronic Branching Fractions and DD Cross Section at ψ (3770) from CLEO c

with the Belle II Analysis Software Framework

Design of the new ATLAS Inner Tracker for the High Luminosity LHC era

(a) (b) Fig. 1 - The LEP/LHC tunnel map and (b) the CERN accelerator system.

1 Introduction The SLAC B Factory asymmetric B-factories was approved by President Clinton in October B-factories The inaugural meeting of the d

arxiv:hep-ex/ v1 31 Dec 2001

e + e - (1) Silicon Vertex Detector

Early physics with the LHCb detector

Linear Collider Workshop 2017, Strasbourg

Weak Decays, CKM, Anders Ryd Cornell University

Alexander Leopold Felicitas Breibeck Christoph Schwanda. for the Belle Collaboration

Radiative and EW Penguin B-Decays with the Belle Detector. Beauty 2003

pp physics, RWTH, WS 2003/04, T.Hebbeker

Current status and results of the experiments at VEPP-2000

Particle detection 1

Non-collision Background Monitoring Using the Semi-Conductor Tracker of ATLAS at LHC

Physics Prospects at Belle II. Jake Benne(, Carnegie Mellon University June 18, 2016 BEACH Fairfax, VA

Results from B-Physics (LHCb, BELLE)

Yiming Li (LAL, Orsay) On behalf of the LHCb and MoEDAL collaborations

Marcello A. Giorgi. Università di Pisa & INFN Pisa La Biodola May 30, 2011 XVII SuperB Workshop and Kick off Meeting

The LHCb Upgrade. Status of LHCb The pre upgrade years. Running scenario A few selected channels.

CMS Note Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland

Measurement of Collins Asymmetries in the inclusive production of hadron pairs

The LHCb Upgrade and beyond

arxiv: v1 [hep-ex] 2 Dec 2010

PoS(Vertex 2016)004. ATLAS IBL operational experience

CESR and CLEO. Lepton Photon 99 Klaus Honscheid Ohio State University. Klaus Honscheid, LP 99 1

Status of LHCb and Physics Prospects

Cracking the Unitarity Triangle

Prospects for Detecting Local Parity Violating Effects in Quark Fragmentation at. and

Hiroyuki Sagawa KEK OHO 1-1, Tsukuba, Ibaraki, Japan

Lecture 8. Detectors for Ionizing Particles

Dark Matter Search with Belle II

Expected Performance of the ATLAS Inner Tracker at the High-Luminosity LHC

The LHCb Experiment II Detector XXXIV SLAC Summer Institute, July, 2006

LHCb Overview. Barbara Storaci on behalf of the LHCb Collaboration

ATLAS New Small Wheel Phase I Upgrade: Detector and Electronics Performance Analysis

Study of Edgeless TimePix Pixel Devices. Dylan Hsu Syracuse University 4/30/2014

Modulations of the di-pion pair x- section at Belle (and the future of FF measurements at BelleII)

The Full Event Interpretation for Belle II. Masterarbeit

CESR and CLEO. 1 Introduction. Klaus Honscheid Department of Physics Ohio State University Columbus, Ohio 43210

Identifying Particle Trajectories in CMS using the Long Barrel Geometry

The BaBar Detectorat theslac B-Factory

READINESS OF THE CMS DETECTOR FOR FIRST DATA

LHCb results and prospects

The ATLAS Silicon Microstrip Tracker

Top Physics at CMS. Intae Yu. Sungkyunkwan University (SKKU), Korea Yonsei University, Sep 12 th, 2013

Aerogel RICH counter for the Belle II forward PID

Belle/Belle2. 1.Jul.2011

Design and Simulation of Beam-Background Monitors in the Vicinity of the Electromagnetic Calorimeter for the Belle II Experiment

A-Exam: The Rare B s µ + µ decay and tanβ

The LHCb Flavour Physics Experiment

Transcription:

Prospects and Status of Belle II experiment Yoshiyuki Onuki High Energy Physics group The 3rd Tohoku University GCOE International Symposium 1

Outline KEKB and Belle experiment Physics motivation for Belle2 experiment SuperKEKB accelerator Belle2 detector Contributions from Tohoku University Construction schedule 2

Quark transition coupling constant in SM u c t V CKM : Cabibbo-Kobayashi- Maskawa Matrix d s b V CKM V CKM =1 f 3 arg V udv ub * V cd V cb * (0,0) V ud V ub* V cd V cb* f 3 (r,h) f 2 V td V tb* V cd V cb* f 1 (1,0) B-meson system is the best place to measure the matrix elements 3 since the three sides of the bottom related triangle is same order of magnitude.

KEKB e + e collider and Belle detector KEKB ~1 km in diameter Mt. Tsukuba Belle 8 GeV e - and 3.5 GeV e + collided on resonance of Y(4S)~10.58GeV Y(4S) consists of bounding state of bottom and unti-bottom quark and almost all Y(4S) decay into B-meson and anti B-meson pair. 15countries,63 institutes,429people L peak = 2.1 x 10 34 sec -1 cm -2 >Twice of the design Luminosity! Producing enormous BB pairs copiously called B-factory Detecting the produced particles and reconstruct the interaction by Belle 4

The last beam abort of KEKB on June 30, 2010 First physics run on June 2, 1999 Last physics run on June 30, 2010 L peak = 2.1x10 34 /cm 2 /s L > 1ab -1 Corresponds to 1.1 Billion BB pairs! 5

Physics outputs from Belle Established the mixing-induced time-dependent CP violation(tcpv) with B 0 J/yK S and related decays in 2002. This provides sin2f 1. No.55 Yutaro Sato Study of B-pi tagging method at the Y(5S) resonance for the measurement of CP-violation parameter sin2f1 Measured TCPV of B 0 fk S and related penguin-dominated decays Discovered a new resonance named X(3872) and exotic hadrons. The studies cotributes nuclear physics. Measured f3, an angle of CKM unitary triangle, with various methods No.53 Yasuyuki Horii First Evidence of the Suppressed B Meson Decay B - DK -, D K + p - No.5 Kennosuke Itagaki Study of the B D*pi decay for CP violation measurement No.23 Zenmei Suzuki Study of decay B->DK,D->KsKpi for the measurement of the CP-violating angle phi3 6

Motivation for upgrade To observe beyond the Standard Model phenomena, New physics contribution via Tunnel effect using penguin-dominant decays b sss transition b sg,sll transition B tn decay At the same time, well constrained CKM unitary triangle works as the Standard Model reference 7

b sss transition S J/yKs =sin2f 1 DS fks S fks -S J/yKs In SM, DS fks ~0 DS fks 0 indicates NP Experimental determination of DS fks can constraint flavor violation in SUSY model under the some approximation. 8

b sg&sll transition Model independent new physics search Both mode can compare SM model prediction with experimental measurements. For example: Forward backward asymmetry in B K*l + l - 657 million BB pairs arxiv:0810.0335 Belle collaboration I.Adachi et al. The solid (dashed) curve shows the SM (C 7 = C SM 7 ) prediction. 9

KEKB and Belle upgrade plan 10

KEKB to SuperKEKB SuperKEKB 10 36 40 times higher luminosity KEKB Next generation B-factories 11 E.Kikutani / M. Masuzawa

Strategies for increasing Luminosity (1) Smaller b y * (2) Increase beam currents Nano-Beam scheme (3) Increase x y Collision with very small spot-size beams 12

SuperKEKB collider e + 4GeV 3.6 A Belle II Colliding bunches New beam pipe & bellows e - 7GeV 2.6 A SuperKEKB New IR New superconducting /permanent final focusing quads near the IP Replace short dipoles with longer ones (LER) Redesign the lattices of HER & LER to squeeze the emittance Low emittance positrons to inject Damping ring Add / modify RF systems for higher beam current Positron source New positron target / capture section TiN-coated beam pipe with antechambers Low emittance gun Low emittance electrons to inject Target: L = 8x10 35 /cm 2 /s 13

How to reconstruct B-meson:B 0 J/yK S PID ECL KLM Extrapolate tracks from outer to inner detector Particle identification Energy measurement CDC Reconstruction of charged particle Determination of the momentum SVD Insert tracks to the Silicon Vertex Detector Determine energy and momentum and vertex in each particle 14

Belle to Belle II upgrade SVD: 4 DSSD lyrs g 2 DEPFET lyrs + 4 DSSD lyrs CDC: small cell, long lever arm ACC+TOF g TOP+A-RICH ECL: waveform sampling (+pure CsI for end-caps) KLM: RPC g Scintillator +MPPC(end-caps) 15

DEPFET pixel detector(pxd) DEPFET pixel detector: Baseline for innermost pixel Acceptance Radiation tolerance Radiation length Hit occupancy 17 <θ<150 >10MRad 0.16%/layer 1-2%(layer1) 16

DEPFET(DEPleted Field Effect Transistor) Full depleted Bulk CMOS. Electron-hole pairs generated by charged Particle accumulates in the Internal gate. Electric field generates between Gate Internal gate The situation is as same as applying Gate voltage in the MOSFET. Drain-Souce current I ds is flowing. Instead of readout electron-hole pair, readout DI ds of MOSFET A full depleted MOSFET with Internal gate acts like a pixel detector(50mm 56mm 50mm) 17

Silicon strip vertex detector(svd) Acceptance 17 <θ<150 Radiation tolerance Radiation length 30MRad ~0.58%/layer Hit occupancy 6.7%(layer3) 6 DSSD 187 DSSDs rf- strips e e 1D+1D strip sensor acts as 2D detector z- strips h h Double Sided Strip Detector (DSSD) 18

Origami module Flexible print circuit board Conventional readout scheme(belle) R/O chips in both side Bonding wires rf- strip z- strip APV25 Doesn t work in Belle2@40 times Lum. of Belle Origami readout scheme(belle2) - Replacing fast R/O chip: VA1TA APV25 - Adapting chip on sensor method for S/N - Realizing one side readout to extract the other side readout wrapping DSSD with Flex PCB. Flexible print circuit board Bonding wire Rohacell DSSD 19

Central Drift Chamber longer lever arm improve resolution of momentum and de/dx Belle Belle Belle II inner most sense wire r=88mm r=168mm outer most sense wire r=863mm r=1111.4mm Number of layers 50 56 Total sense wires 8400 14336 Belle II small cell normal cell Gas He:C2H6 He:C2H6 sense wire W(Φ30μm) W(Φ30μm) field wire Al(Φ120μm) Al(Φ120μm) 10 mm 6~8 mm 18 mm 10~20 mm 20

Particle Identification(PID) Detector Time of Projection chamber(top) Threshold type Cherenkov PID(Belle) Quartz RICH PID for barrel Aerogel RICH type PID for endcap RICH with Time measurement TTS~40ps Aerogel Ring image Cherenkov(ARICH) 200mm 200mm Aerogel radiator n~1.05 Hamamatsu HAPD + new ASIC 21

Contributions from Tohoku University group Beam BG study in beam interaction region SVD vertex detector construction SOI(Silicon On Insulator) pixel detector for future PXD option Beam BG study by K.Nakano&H.Yamamoto SOI beam test study by H.Katsurayama SOI radiation tolerance study by Y.Ono SVD development by me & Y.Himori 22

Construction Schedule of SuperKEKB/Belle II FY2009 FY2010 FY2011 FY2012 FY2013 FY2014 Linac e+ new matching & L-band acc. R&D Construction RF-gun & laser system Design study Commissioning at test stand Damping Ring R&D, Design Mass Fabrication Tunnel construction Building construction Installation Main Ring Building construction R&D, Design Mass Fabrication Installation Belle II Detector R&D Construction Mass Production Installation 23 Cosmic Ray Test

Peak Luminosity (cm -2 s -1 ) Integrated Luminosity (ab -1 ) Luminosity upgrade projection Milestone of SuperKEKB 9 month/year 20 days/month We will reach 50 ab -1 in 2020~2021. Commissioning starts mid of 2014 Shutdown for upgrade FY 24

Summary KEKB&Belle upgrade project was approved The target is 40 times luminosity of KEKB and 50 times data of Belle. The motivation is to observe beyond standard model in particle physics. Tohoku group contributes beam BG study in IR, SVD and SOI pixel detector for future upgrade option. The experiment will start in 2014 25

Funding Status 10 billion yen funded by Very Advanced Research Support Program of MEXT(Ministry of Education, Culture, Sports, Science and Technology) in FY2010-2012 KEKB upgrade has been approved. Construction had started. 26

SOI pixel detector for PXD option Silicon On Insulator(SOI) pixel detector - Next generation pixel detector R/O electronics and sensor in single wafer =>Monolithic detector. -Able to implement sophisticated functions in Front End Electronics. e.g. counter, memory -Developed by KEK and Tohoku Univ etc. -Manufacturer is OKI-Semiconductor Miyagi e+ beam test@tohoku LNS 27

28