|
|
|
- Esmond Cain
- 5 years ago
- Views:
Transcription
1
2
3
4
5
6 µ µ à e ν ν µ + ( A, Z) à ν µ + (A,Z 1) µ +(A, Z) à e +(A,Z)
7 SINDRUM II µ Rext= number of proton between pulses number of proton in a pulse
8 capture in the moderator (see also Fig.3.1 and the discussion in the text). e m t 10 3 run2000 on gold SINDRUM II measurement µe2ν simulation µe simulation at B=10-11 a i a events / 100 kev t F f o 1 T ETOT (MeV) N w
9
10
11 パイ中間子生成標的 ミューオン輸送磁石 陽子ビーム ミューオン静止標的 パイ中間子捕獲磁石 電子輸送磁石 電子 パイ中間子 ミューオン 電子検出器 - 検出器ソレノイド磁石 - ストローチューブ飛跡検出器 - LYSO カロリメーター
12 New and accelerator research facility, using MW-class high power proton beams at both 3 GeV and 30 GeV. J-PARC Tokai KEK Tsukuba
13 LINAC 400 MeV Neutrino beam to Kamioka Rapid Cycle Synchrotron Material and Life Science Facility Nuclear and Particle Physics Exp. Hall Energy : 3 GeV Repetition : 25 Hz Design Power : 1 MW Main Ring Max Energy : 30 GeV Design Power for FX : 0.75 MW Expected Power for SX : > 0.1 MW
14
15
16 Proton beam Pion production target Radiation shield Muon beam transport solenoid Matching solenoid Capture solenoid COMET Solenoids and Detectors for the CDR version Late-arriving particle tagger Beam collimator Muon stopping target Muon target solenoid Beam blocker DIO blocker Calorimeter Tracker Detector solenoid Curved sepctrometer solenoid Figure 5.14: Present design of the solenoid channel used in the tracking studies Dipole fields for drift compensation To keep the center of the helical trajectories of the muons with reference momentum p 0 in the bending plane, a compensating vertical dipole field should be applied. The magnitude of the compensating dipole field is given by B comp = 1 ( p 0 cos θ ), (5.6) qr 2 cos θ 0
17
18 δδ
19
20 Switch Yard Beamline Elements A-Line B-Line Beam line component installation in progress in SY since 2014 Beam transport line in HD hall SC magnets Hall construction He compressor used for E36 will be reused for COMET Significant construction work 2016 Summer to connect SY and Hall along the B-Line 90 deg. Transport Solenoid installed in Spring 2015 COMET Hall ready in Spring 2015
21 All geometry implemented in the full simulation: ICEDUST Detector for physics measurement in Phase I CDC : the main detector of COMET Phase-I Physics Beam PSI 2015 Trigger Hodoscope Counter Scintillator + Cerenkov Analysis algorithm development in progress using simulation data. ex) track finding in CyDET Wire stringing completed in July 2016 at KEK CDC Read Out Electronics RECBE production at IHEP
22 CDC Construction COMET Phase-I Physics Main Detector Wire stringing completed in July st cosmic-ray event observed in Sep. 2016
23 Straw tracker (operational in vacuum) prototype Detector for beam BG measurement in Phase I and physics measurement in Phase II ECal (LYSO) R&D using prototypes 100 MeV electron Ecal Pile-up study using simulation data Crystal quality test bench at JINR Wave form taken in the test ß Electron beam test at ELPH Ecal PID performance evaluation at PSI 2015
24
25 opportunities for cooperation with Mu2e M C C AlCap@PSI C M Dec. 13 M C M M C C M C C M COMET Mu2e
26
27
28 DeeMe
29 DeeMe
30 Acceptance (sr/mev/c) 0.25 From a Target 40 H-port Frange GV Entrance GV Exit HS2 Entrance HS3 Entrance HSEP Entrance 0.2 HB4 Entrance HB4 Exit HQ2 Entrance Focus Momentum (MeV/c)
31
32
New and accelerator research facility, using MW-class high power proton beams at both 3 GeV and 30 GeV. J-PARC Tokai KEK Tsukuba LINAC 400 MeV Rapid Cycle Synchrotron Energy : 3 GeV Repetition : 25 Hz
COMET muon conversion experiment in J-PARC
Institute for Basic Science, Daejeon, Korea E-mail: myeongjaelee@ibs.re.kr COMET is an experiment at J-PARC, Japan, which will search for neutrinoless conversion of muons into electrons in the field of
Overview of the COMET Phase-I experiment
Overview of the COMET Phase-I experiment Osaka University E-mail: m-wong@kuno-g.phys.sci.osaka-u.ac.jp Charged Lepton Flavour Violation (CLFV) has yet to be observed experimentally. If observed, it would
Experimental Searches for Muon to Electron Conversion
Experimental Searches for Muon to Electron Conversion Yoshitaka Kuno Department of Physics Osaka University May 20th, 2009 FJPPL, EPOCHAL, Tsukuba Outline Overview of Our Proposal to FJPPL Physics Motivation
The Mu2e Transport Solenoid
The Mu2e Transport Solenoid J. Miller Boston University for the Mu2e Collaboration 23 January 2009 1 Mu2e Muon Beamline Requirements Pulsed beam Deliver high flux µ beam to stopping target At FNAL, high
An Overview of the COMET Experiment and Its Recent Progress
An Overview of the COMET Experiment and Its Recent Progress Benjamin E. Krikler Imperial College London (Dated: April 17, 2016) 418 Abstract Forbidden in the Standard Model, Charged Lepton Flavour Violation
Mu2e Experiment at Fermilab
Mu2e Experiment at Fermilab, Yuri Oksuzian Newcomers lunch 1 Mu2e Fermilab is actively pursuing the searches with high intensity beams: NOvA, Shortbaseline neutrino, DUNE, Muon g-2, Mu2e Mu2e will search
MuSIC- RCNP at Osaka University
Commissioning of new DC muon beam line, MuSIC- RCNP at Osaka University Dai Tomono Research Center for Nuclear Physics (RCNP), Osaka University On behalf of the MuSIC- RCNP collaboration tomono@rcnp.osaka-
K + Physics at J-PARC
Takeshi K. Komatsubara (KEK-IPNS) 1 K + Physics at J-PARC K + Physics at J-PARC Takeshi K. Komatsubara (KEK-IPNS) 2005.May.26 K - RARE Meeting at INFN, Frascati Takeshi K. Komatsubara (KEK-IPNS) 2 K +
Muon to Electron Conversion: Experimental Status in Japan and the US
Muon to Electron Conversion: Experimental Status in Japan and the US James P Miller 1 Department of Physics, Boston University 590 Commonwealth Ave., Boston E-mail: miller@bu.edu A description is given
arxiv: v1 [hep-ex] 7 Sep 2016
![arxiv: v1 [hep-ex] 7 Sep 2016](/thumbs/80/82243034.jpg "arxiv: v1 [hep-ex] 7 Sep 2016")
arxiv:1609.02021v1 [hep-ex] 7 Sep 2016 University of Siena and INFN Pisa E-mail: luca.morescalchi@pi.infn.it The Mu2e Experiment at Fermilab will search for the coherent, neutrinoless conversion of muons
The first muon beam from a new high-intensity DC muon source, MuSIC
The first muon beam from a new high-intensity DC muon source, MuSIC Tran Hoai Nam, Department of Physics, Osaka University On behalf of the MuSIC collaboration PANIC11@MIT - July 26th, 2011 1 Outline Mo#va#on
The T2K Neutrino Experiment
The T2K Neutrino Experiment Tokai to Kamioka TPC-Group, Institute 3b Achim Stahl, Stefan Roth, Karim Laihem, Dennis Terhorst, Jochen Steinmann 03.09.2009, Bad Honnef 2009-09-03 1 Overview 1. Neutrinos
Studies of Cylindrical Drift Chamber for COMET Phase-I
Studies of Cylindrical Drift Chamber for COMET Phase-I Speaker: TingSam Wong 1 22 th Feb, 2017 Outline Introduction Studies related to CDC Software studies Track reconstruction Future prospect Summary
PSI. Muon Experiment at the PSI, KEK
PSI Muon Experiment at the PSI, KEK RCNP, 23-24.Feb.2010, RCNP 2 Contents PSI? Muon Beam Line in PSI Muon Experiment in PSI past / present (MEG) Future Prospects in PSI PSI? 4 PSI : Paul Scherrer Institut
Recent Results from Alysia Marino, University of Colorado at Boulder Neutrino Flux Workshop, University of Pittsburgh, Dec 6 8,2012
Recent Results from Alysia Marino, University of Colorado at Boulder Neutrino Flux Workshop, University of Pittsburgh, Dec 6 8,2012 Outline T2K Beamline and Detectors Uncertainties from prior measurements
SSA Measurements with Primary Beam at J-PARC
SSA Measurements with Primary Beam at J-PARC Joint UNM/RBRC Workshop on Orbital Angular Momentum in Albuquerque February 25 th, 2006 Yuji Goto (RIKEN/RBRC) February 25, 2006 Yuji Goto (RIKEN/RBRC) 2 Introduction
How J-PARC recovered from the big earthquake
How J-PARC recovered from the big earthquake KEK / Fujio Naito Outline About J-PARC The earthquake Damage on J-PARC Recovery plan Beam study results Summary J-PARC (Japan Proton Accelerator Research Complex)
Mu2e: Coherent μ e Conversion Experiment at Fermilab. David Brown, LBNL representing the mu2e collaboration
Mu2e: Coherent μ e Conversion Experiment at Fermilab David Brown, LBNL representing the mu2e collaboration Charged Lepton Flavor Violation ν mixing implies Charged Lepton Flavor Violation (CLFV) Predicted
Searching for at Jefferson Lab. Holly Szumila-Vance On behalf of the HPS, APEX, DarkLight, and BDX 2017 JLab User s Group Meeting 20 June 2017
Searching for at Jefferson Lab Holly Szumila-Vance On behalf of the HPS, APEX, DarkLight, and BDX 2017 JLab User s Group Meeting 20 June 2017 Overview: Motivation Dark photon searches: APEX (Hall A) HPS
Status of KEK-E391a and Future Prospects on K L π 0 νν at KEK. GeiYoub Lim IPNS, KEK
Status of KEK-E391a and Future Prospects on K L π 0 νν at KEK GeiYoub Lim IPNS, KEK E391a Collaboration Joint Institute for Nuclear Research (Dubna), Russia High Energy Accelerator Research Organization,
Charged Lepton Flavour Violation:
Charged Lepton Flavour Violation: mu2e, mu3e and Comet Gavin Hesketh, UCL Thanks to Mark Lancaster, Yoshi Uchida, Joost Vossebeld 2 Charged Lepton Flavour Violation () complimentary way to search for new
Lepton Flavour Violation
Lepton Flavour Violation Search for e at Paul Scherrer Institut Satoshi Mihara ICEPP, Univ. of Tokyo http://meg.icepp icepp.s..s.u-tokyo.ac.jp, http://meg.psi psi.ch,http://meg.pi.,http://meg.pi.infn.it
K2K and T2K experiments
K2K and T2K experiments Issei Kato TRIUMF, Canada for the K2K and T2K collaborations Neutrino Oscillation Workshop 2006 at Conca Specchiulla,, Otranto, Italy Outline K2K experiment, shortly What s updated
The Mu2e Experiment at Fermilab
The Mu2e Experiment at Fermilab 1, 2, Kevin R. Lynch (The Fermilab Mu2e Collaboration), 1 Department of Earth and Physical Sciences, York College, City University of New York, 94-20 Guy R. Brewer Blvd,
J-PARC Japan Proton Accelerator Research Complex. J-PARC Status after March 11. J-PARC at Tokai-mura, Ibaraki-ken
J-PARC Japan Proton Accelerator Research Complex J-PARC Status after March 11 J-PARC at Tokai-mura, Ibaraki-ken Bird s eye photo in July 2009 J-PARC Japan Proton Accelerator Research Complex ν to SK 400MeV
SciBar and future K2K physics. F.Sánchez Universitat Aútonoma de Barcelona Institut de Física d'altes Energies
SciBar and future K2K physics F.Sánchez Universitat Aútonoma de Barcelona Institut de Física d'altes Energies ICRR, 29 th October 2003 Outline Introduction: K2K SciBar detector: Physics goals Design Electron
China high-intensity accelerator technology developments for Neutron Sources & ADS
AT/INT-04 China high-intensity accelerator technology developments for Neutron Sources & ADS J. Wei, Tsinghua University, China S.N. Fu, IHEP, CAS, China International Topical Meeting on Nuclear Research
Present Status from the Experimental Study of Neutral Kaon Photoproduction around Threshold Region at Tohoku-LNS
Present Status from the Experimental Study of Neutral Kaon Photoproduction around Threshold Region at Tohoku-LNS Masashi Kaneta for the NKS2 collaboration Department of Physics, Tohoku University Introduction
Masaharu Aoki Osaka University
Muon Particle Physics Masaharu Aoki Osaka University Overview Introduction Static Properties Muon g-2 Muon EDM Dynamic Properties Lepton Flavor Violations e (MEG), e conversion (MECO,PRISM) Michel parameters
Particle Energy Loss in Matter
Particle Energy Loss in Matter Charged particles loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can be described for moderately
PULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC
THO3AB3 Proceedings of HB, East-Lansing, MI, USA PULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC P.K. Saha, H. Harada, H. Hotchi and T. Takayanagi J-PARC
arxiv: v1 [physics.ins-det] 26 Sep 2018
![arxiv: v1 [physics.ins-det] 26 Sep 2018](/thumbs/89/99396108.jpg "arxiv: v1 [physics.ins-det] 26 Sep 2018")
SNSN-???-?? September 27, 2018 Latest Updates from the AlCap Experiment arxiv:1809.10122v1 [physics.ins-det] 26 Sep 2018 Andrew Edmonds on behalf of the AlCap Collaboration Lawrence Berkeley National Laboratory,
clfv searches using DC muon beam at PSI
KEK IPNS, J-PARC Center, and Sokendai E-mail: satoshi.mihara@kek.jp Search for lepton-flavor violation in the charged lepton sector (clfv) is a clue to new physics beyond the Standard Model. MEG experiment
HypTPC for high-rate beams
HypTPC for high-rate beams 佐甲博之 ( 原子力機構 ) 新学術領域 中性子星核物質 第 2 回検出器ワークショップ 2017/3/4, 東工大 1 Outline HypTPC の設計 The TPC vs HypTPC High rateへの対応 Field cageの帯電対策 HypTPC,TPCの応用 2 TPC The best three-dimensional
Particle Acceleration
Nuclear and Particle Physics Junior Honours: Particle Physics Lecture 4: Accelerators and Detectors February 19th 2007 Particle Beams and Accelerators Particle Physics Labs Accelerators Synchrotron Radiation
Intense Slow Muon Physics
1 Intense Slow Muon Physics Yoshitaka Kuno a a Department of Physics, Osaka University, Toyonaka, Osaka 560-0043, Japan Physics programs with slow muons at a neutrino factory are described. Emphasis is
Appendix A2. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France.
Appendix A. Particle Accelerators and Detectors The Large Hadron Collider (LHC) in Geneva, Switzerland on the Border of France. Prepared by: Arash Akbari-Sharbaf Why Build Accelerators? Probe deeper From
Marcos Dracos IPHC-IN2P3/CNRS Strasbourg. 2 December 2008 M. Dracos, BENE 1
Marcos Dracos IPHC-IN2P3/CNRS Strasbourg 2 December 2008 M. Dracos, BENE 1 Staging neutrino facilities towards the NF Cover "high" 13 range Cost effective facility Low intensity SPL already approved, Detector
The DAΦNE Beam Test Facility
The DAΦNE Beam Test Facility Giovanni Mazzitelli & Paolo Valente Laboratori Nazionali di Frascati Overview BTF Parameters BTF operation mode Commissioning results First users experience Future plans Introduction
The Mu3e PSI
The Mu3e Experiment @ PSI searching for the neutrinoless muon decay m + e + e - e + Tau 2016 Beijing, Sept. 23, 2016 Alessandro Bravar for the Mu3e Collaboration LFV in Standard Model Flavor Conservation
PoS(NOW2016)003. T2K oscillation results. Lorenzo Magaletti. INFN Sezione di Bari
INFN Sezione di Bari E-mail: lorenzo.magaletti@ba.infn.it The TK (Tokai-to-Kamioka) experiment is a second generation long baseline neutrino oscillation experiment that probes physics beyond the Standard
Neutrino beamline prospects, concepts Milorad Popovic
NuFact 2016 Neutrino beamline prospects, concepts Milorad Popovic APC- Fermilab, Batavia, IL 60510, USA August, 21, 2016 1 M. Popovic Conventional Neutrino Beamline 2 M. Popovic Conventional Neutrino Beamline
PoS(NuFact2017)088. EMuS in CSNS. Guang Zhao 1. Institute of High Energy Physics Beijing, China
1 Institute of High Energy Physics Beijing, China E-mail: zhaog@ihep.ac.cn In this presentation, we report the recent progress in EMuS at CSNS. The following topics will be discussed: a) the base design
IPBI-TN June 30, 2004
Spray Electron Beam for Tests of Linear Collider Forward Calorimeter Detectors in SLAC End Station A R. Arnold UMass Amherst, Amherst MA 01003 T. Fieguth Stanford Linear Accelerator Center Menlo Park,
MINOS. Physics Program and Construction Status. Karol Lang The University of Texas at Austin. YITP: Neutrinos and Implications for Physics Beyond
MINOS Physics Program and Construction Status Karol Lang The University of Texas at Austin YITP: Neutrinos and Implications for Physics Beyond YITP Conference: Neutrinos and Implications The Standard for
Particle Energy Loss in Matter
Particle Energy Loss in Matter Charged particles, except electrons, loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can
LFV with µ-beams: status and perspectives
LFV with µ-beams: status and perspectives Donato Nicolò Università di Pisa & INFN XXXX Rencontres de Moriond 5-12 March 2005 Outline Theoretical issues for LFV SUSY predictions Connections with neutrino
Reaction measurement Instrument ANNRI. Hideo Harada. Research Group for Applied Nuclear Physics. 5th ASRC 2012 at Tokai
J PARC and Accurate Neutron Nucleus Nucleus Reaction measurement Instrument ANNRI Hideo Harada Research Group for Applied Nuclear Physics Japan Atomic Energy Agency (JAEA) 1 What is the J PARC? J PARC
Operational Experience with J-PARC Injection and Extraction Systems
Operational Experience with J-PARC Injection and Extraction Systems Pranab Kumar Saha Japan Proton Accelerator Research Complex (J-PARC) 46th ICFA Advanced Beam Dynamics Workshop ( HB2010 ) Morschach,
Test Beams: Availability & Plans
Gene Fisk Fermilab LCWS_2002 Jeju Do Test Beams: Availability & Plans KEK DESY CERN Fermilab SLAC Other KEK Test Beams @ 12 GeV PS Information from: yoshiaki.fujii@kek.jp KEK East Counter Hall T1 and π2
Lucite Hodoscope for SANE
Lucite Hodoscope for SANE A. Ahmidouch, S. Danagoulian NC A&T State University Outline Cosmic Ray test of a lucite prototype bar The old result from Monte Carlo Geometry consideration Trigger Electronics
CLAS12 at Jefferson Lab
CLAS12 at Jefferson Lab Daria Sokhan University of Glasgow, UK IPPP/NuSTEC Topical Meeting on Neutrino-Nucleus Scattering IPPP, Durham, UK 19 April 2017 Jefferson Lab 6 GeV era Jefferson Lab CEBAF: Continuous
Update from the Mu3e Experiment
Update from the Mu3e Experiment Niklaus Berger Physics Institute, University of Heidelberg Charged Lepton Working Group, February 2013 Overview The Challenge: Finding one in 10 16 muon decays The Technology:
NEUTRINO FACTORY / MUON STORAGE RING
NEUTRINO FACTORY / MUON STORAGE RING ANIMESH CHATTERJEE INO STUDENT Content What is Neutrino Factory Why We need Neutrino Factory Details of Neutrino Factory Detector for different Channel Neutrino Factory
AIM AIM. Study of Rare Interactions. Discovery of New High Mass Particles. Energy 500GeV High precision Lots of events (high luminosity) Requirements
AIM AIM Discovery of New High Mass Particles Requirements Centre-of-Mass energy > 1000GeV High Coverage Study of Rare Interactions Requirements Energy 500GeV High precision Lots of events (high luminosity)
Particle and Nuclear Physics Facilities A summary of approved experiments. K. Nishikawa KEK June 5, 2008
Particle and Nuclear Physics Facilities A summary of approved experiments K. Nishikawa KEK June 5, 2008 1 Two stage aapproval The stage-1 approval This will be given by the IPNS director based on the recommendation
COMET Satoshi MIHARA IPNS, KEK
COMET Satoshi MIHARA IPNS, KEK Outline clfv search experiment COMET at J-PARC Physics Goal Requirement Summary clfv Search Experiments muon g-2 Neutrino Oscillation Higgs boson New Physics BSM clfv Search
Particle Detectors A brief introduction with emphasis on high energy physics applications
Particle Detectors A brief introduction with emphasis on high energy physics applications TRIUMF Summer Institute 2006 July 10-21 2006 Lecture I measurement of ionization and position Lecture II scintillation
First neutrino beam and cosmic tracks. GDR neutrino
Magali Besnier T2K status tt of the experiment First neutrino beam and cosmic tracks GDR neutrino 28 04 09 T2K Tokai 2 Kamiokande Main goals : 1) Measurement of 13 mixing angle studying the e oscillation
Atsushi Sakaguchi (Osaka University) for the J-PARC E10 Collaboration
Atsushi Sakaguchi (Osaka University) for the J-PARC E10 Collaboration Study of Λ hypernuclei and ΛN interaction Λ hypernucleus System made of a Λ hyperon and a nucleus(a) ΛN interaction strong enough to
On the possible construction of a Mu2e calibration linac built around a spare Project-X or ILC cryomodule
On the possible construction of a Mu2e calibration linac built around a spare Project-X or ILC cryomodule George Gollin a Department of Physics University of Illinois at Urbana-Champaign 1110 West Green
Marcos Dracos IPHC, Université de Strasbourg, CNRS/IN2P3, F Strasbourg, France
Neutrino CP Violation with the ESSνSB project IPHC, Université de Strasbourg, CNRS/INP3, F-603 Strasbourg, France E-mail: marcos.dracos@inp3.fr After measuring in 01 a relatively large value of the neutrino
NA62: Ultra-Rare Kaon Decays
NA62: Ultra-Rare Kaon Decays Phil Rubin George Mason University For the NA62 Collaboration November 10, 2011 The primary goal of the experiment is to reconstruct more than 100 K + π + ν ν events, over
Figure 1 Overview of the T2K experiment
Figure 1 Overview of the T2K experiment The proton beams extracted from the main ring synchrotron at J-PARC are directed in a westward direction through the T2K primary beam line. The beams strike a target
LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration
LCS2014 International Workshop LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration Outline Overview of the LEPS&LEPS2 beamlines Recent results from LEPS Search
Near detector tracker concepts. D. Karlen / U. Vic. & TRIUMF T2K ND280m meeting August 22, 2004
Near detector tracker concepts D. Karlen / U. Vic. & TRIUMF T2K ND280m meeting August 22, 2004 Longitudinal extent of tracker modules Consensus has developed that the near detector should consist of a
A beam line for schools
A beam line for schools Great things can happen when high schools get involved with cutting edge science, and that s exactly what CERN is proposing with its new beam line for schools competition, which
Examples for experiments that can be done at the T9 beam line
Examples for experiments that can be done at the T9 beam line Example 1: Use muon tomography to look for hidden chambers in pyramids (2016 winning proposal, Pyramid hunters) You may know computer tomography
Information about the T9 beam line and experimental facilities
Information about the T9 beam line and experimental facilities The incoming proton beam from the PS accelerator impinges on the North target and thus produces the particles for the T9 beam line. The collisions
Low slice emittance preservation during bunch compression
Low slice emittance preservation during bunch compression S. Bettoni M. Aiba, B. Beutner, M. Pedrozzi, E. Prat, S. Reiche, T. Schietinger Outline. Introduction. Experimental studies a. Measurement procedure
STATUS REPORT ON SURVEY AND ALIGNMENT OF J-PARC AFTER THE EARTHQUAKE
STATUS REPORT ON SURVEY AND ALIGNMENT OF J-PARC AFTER THE EARTHQUAKE N. Tani#, T. Morishita, S. Meigo, M. Harada, H. Stefanus, JAEA/J-PARC, Tokai, Japan M. Shirakata, T. Ishii, Y. Fujii, Y. Shirakabe,
J-PARC μ-e --- PRISM/Phase-1 ---
J-PARC μ-e --- PRISM/Phase-1 --- Masaharu Aoki Osaka U. ICEPP, 2007/11/06 Lepton Flavor Violation μ-lfv (SIMDRUM II) μ-e MECO, mu2e and PRISM/Phase-1 PRISM/Phase-1 @ J-PARC Lepton Flavor Mixing Quark Mixing
Reactor & Spallation Neutron Sources
Reactor & Spallation Neutron Sources Oxford School of Neutron Scattering Oxford, 2011-09-06 Ken Andersen ESS Instruments Division ISIS ILL Time evolution: Major neutron sources ILL BENSC (D) SINQ (CH)
PHYS 5326 Lecture #2. Wednesday, Jan. 24, 2007 Dr. Jae Yu. Wednesday, Jan. 24, 2007 PHYS 5326, Spring 2007 Jae Yu
PHYS 5326 Lecture #2 Wednesday, Jan. 24, 2007 Dr. 1. Sources of Neutrinos 2. How is neutrino beam produced? 3. Physics with neutrino experiments 4. Characteristics of accelerator based neutrino experiments
LHC Status and CERN s future plans. Lyn Evans
LHC Status and CERN s future plans Lyn Evans Machine layout L. Evans EDMS document no. 859415 2 Cryodipole overview 1250 1000 Equivalent dipoles 750 500 250 0 01-Jan-01 01-Jan-02 01-Jan-03 01-Jan-04 01-Jan-05
The First Large Application of MPPC: T2K Neutrino Beam Monitor INGRID
The First Large Application of MPPC: T2K Neutrino Beam Monitor INGRID Kyoto University, Japan E-mail: masashi.o@scphys.kyoto-u.ac.jp We report design and performance of T2K neutrino beam monitor INGRID.
Neutrino mixing II. Can ν e ν µ ν τ? If this happens:
Can ν e ν µ ν τ? If this happens: Neutrino mixing II neutrinos have mass (though there are some subtleties involving the MSW mechanism) physics beyond the (perturbative) Standard Model participates Outline:
Lecture 8. CPT theorem and CP violation
Lecture 8 CPT theorem and CP violation We have seen that although both charge conjugation and parity are violated in weak interactions, the combination of the two CP turns left-handed antimuon onto right-handed
Front end, linac upgrade, and commissioning of J-PARC. Y. Liu KEK/J-PARC, Japan
KEK Front end, linac upgrade, and commissioning of J-PARC j-parc Y. Liu KEK/J-PARC, Japan ICFA mini-workshop on Beam Commissioning for High Intensity Accelerators Dongguan, China, June 8-10, 2015 Outlines
Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders
Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Explanation of the Basic Principles and Goals Visit to the CTF3 Installation Roger Ruber Collider History p p hadron collider
HARP (Hadron Production) Experiment at CERN
HARP (Hadron Production) Experiment at CERN 2nd Summer School On Particle Accelerators And Detectors 18-24 Sep 2006, Bodrum, Turkey Aysel Kayιş Topaksu Çukurova Üniversitesi, ADANA Outline The Physics
Study of Neutral Kaon Photo-Production at LNS-Tohoku
Research Report of Laboratory of Nuclear Seience, Tohoku University Vol. 41 (2008) 1 (LNS Experiment : #2552, #2565) Study of Neutral Kaon Photo-Production at LNS-Tohoku P. Bydžovský 1, N. Chiga 2, Y.
Dark Matter Searches with AMS-02. AMS: Alpha Magnetic Spectrometer
Dark Matter Searches with AMS-02 AMS: Alpha Magnetic Spectrometer 2007/2008 Wim de Boer on behalf of the AMS collaboration University of Karlsruhe July, 20. 2004 COSPAR, Paris, W. de Boer, Univ. Karlsruhe
Experimental Methods of Particle Physics
Experimental Methods of Particle Physics (PHY461) Fall 015 Olaf Steinkamp 36-J- olafs@physik.uzh.ch 044 63 55763 Overview 1) Introduction / motivation measurement of particle momenta: magnetic field early
LHCb collaboration. WELCOME to PNPI
LHCb collaboration WELCOME to PNPI Petersbourg Nuclear Physics Iinstitute Russian Academy of Sciences Research directions High energy physics Nuclear physics Solid state physics Molecular biophysics Theoretical
JAPAN PROTON ACCELERATOR RESEARCH COMPLEX
J-PARC JAPAN PROTON ACCELERATOR RESEARCH COMPLEX Facilities at J-PARC The J PARC stands for Japan Proton Accelerator Research Complex and it is a new and exciting accelerator research facility in Japan.
Emittance Measurement in the Muon Ionization Cooling Experiment
Emittance Measurement in the Muon Ionization Cooling Experiment Department of Physics, Imperial College London E-mail: v.blackmore@imperial.ac.uk The Muon Ionization Cooling Experiment (MICE) collaboration
Neutrino Physics. Neutron Detector in the Aberdeen Tunnel Underground Laboratory. The Daya Bay Experiment. Significance of θ 13
Neutrino Physics Neutron Detector in the Aberdeen Tunnel Underground Laboratory John K.C. Leung Department of Physics, HKU On behalf of CUHK, LBL & IHEP Presented to HKRPS on June 21, 2007 Neutrinos have
The Hermes Recoil Silicon Detector
The Hermes Recoil Silicon Detector Introduction Detector design considerations Silicon detector overview TIGRE microstrip sensors Readout electronics Test beam results Vertex 2002 J. Stewart DESY Zeuthen
MTV - S1183 Beam Time Summary. Performance test of MTV new detector : CDC. Yumi Totsuka. Department of Physics, Rikkyo University, Tokyo, Japan
MTV - S1183 Beam Time Summary Performance test of MTV new detector : CDC Yumi Totsuka Department of Physics, Rikkyo University, Tokyo, Japan TRIUMF-ISAC Science Forum (30. Nov. 2011) Schedule: Beam Time
Recent T2K results on CP violation in the lepton sector
Recent T2K results on CP violation in the lepton sector presented by Per Jonsson Imperial College London On Behalf of the T2K Collaboration, December 14-20 2016, Fort Lauderdale, USA. Outline Neutrino
STATUS OF THE J-PARC FACILITY
STATUS OF THE J-PARC FACILITY Shoji Nagamiya, J-PARC Center, 2-4 Shirakata Shirane, Tokai-Mura, Ibaraki 319-1195, Japan Abstract J-PARC (Japan Proton Accelerator Research Complex) consists of three accelerators
The calorimeter project for the Mu2e experiment
The calorimeter project for the Mu2e experiment M. Cordelli, S.Giovannella, F. Happacher, A. Lucà, S.Miscetti, A. Saputi, I. Sarra, G. Pileggi, B. Ponzio Laboratori Nazionali di Frascati of INFN, Frascati,
Hadron Physics with Photon Beam at LEPS/ LEPS2 Takashi Nakano (RCNP, Osaka Univ.) HHIQCD2015, March 3rd, 2015
Hadron Physics with Photon Beam at LEPS/ LEPS2 Takashi Nakano (RCNP, Osaka Univ.) HHIQCD2015, March 3rd, 2015 1 Outline LEPS Overview Some recent results LEPS2 Physics Motivation Overview First experiment
arxiv: v1 [physics.ins-det] 1 Sep 2009
![arxiv: v1 [physics.ins-det] 1 Sep 2009](/thumbs/92/109075179.jpg "arxiv: v1 [physics.ins-det] 1 Sep 2009")
The MEG Spectrometer at PSI Paolo Walter Cattaneo on behalf of the MEG collaboration INFN Pavia, Via Bassi 6, Pavia, I-27100, Italy arxiv:0909.0199v1 [physics.ins-det] 1 Sep 2009 The MEG experiment is
SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland
SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland Michael Böge 1 SLS Team at PSI Michael Böge 2 Layout of the SLS Linac, Transferlines Booster Storage Ring (SR) Beamlines and Insertion Devices
Why do we accelerate particles?
Why do we accelerate particles? (1) To take existing objects apart 1803 J. Dalton s indivisible atom atoms of one element can combine with atoms of other element to make compounds, e.g. water is made of
Fall Quarter 2010 UCSB Physics 225A & UCSD Physics 214 Homework 1
Fall Quarter 2010 UCSB Physics 225A & UCSD Physics 214 Homework 1 Problem 2 has nothing to do with what we have done in class. It introduces somewhat strange coordinates called rapidity and pseudorapidity
Lepton Flavor Violation Experimental Overview
Lepton Flavor Violation Experimental Overview Masaharu Aoki Osaka U. APPEAL07 KEK 2007/2/19-21 Contents Introduction τ-decay experiments μ eγ experiment : MEG μ-e Conversion : MECO, mu2e and PRISM/Phase-1