Giovanni Onorato Fermilab University of Rome “Guglielmo Marconi” INFN Lecce Mu2e general presentation.

Slides:



Advertisements
Similar presentations
ACHIEVEMENTS OF THE TEVATRON FIXED-TARGET PROGRAM Heidi Schellman Northwestern University 1 6/11/12.
Advertisements

Mu2e experiment at Fermilab
F ERMILAB T EST B EAM F ACILITY Aria Soha March 17, 2011.
Calorimetry and Showers Learning Objectives Understand the basic operation of a calorimeter (Measure the energy of a particle, and in the process, destroy.
An accelerator beam of muon neutrinos is manufactured at the Fermi Laboratory in Illinois, USA. The neutrino beam spectrum is sampled by two detectors:
Neutral Particles. Neutrons Neutrons are like neutral protons. –Mass is 1% larger –Interacts strongly Neutral charge complicates detection Neutron lifetime.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
The COherent Muon to Electron Transition (COMET) Experiment
MICE: The International Muon Ionization Cooling Experiment Diagnostic Systems Tracker Cherenkov Detector Time of Flight Counters Calorimeter Terry Hart.
Detecting Particles Martin Gallacher – University of Birmingham.
What we did: ★ Inquiry based calibration data analysis of J/psi meson, W and Z bosons ★ Tours: webtour of CMS, LINAC, Accelerator Control room, DØ, MINOS,
Mu2e: A Proposal for a Muon to Electron Conversion Experiment at FERMILAB James Miller, Boston University CERN, October 2006.
March 2011Particle and Nuclear Physics,1 Experimental tools accelerators particle interactions with matter detectors.
Ivan Logashenko for Mu2e Collaboration
 A GEANT4-based simulation was performed of the production target, solenoid, selection channel, and spectrometer.  The acceptance was found to be 8.3x10.
The Mu2e experiment Zhengyun You University of California, Irvine (for the Mu2e Collaboration) 08/21/2013.
Conveneers: M. Grassi (INFN, Pisa), K. Ishida (RIKEN), Y. Semertzidis (BNL) Summary of WG4, Part Two. Yannis Semertzidis, BNL 1 August, 2004 Most muon.
PRISM and Neutrino Factory in Japan Y. Kuno KEK, IPNS January 19th, 2000 at CERN.
1 Muon Physics Project X Workshop Fermilab 17 November 2007.
Mu2e Experiment and Issues Rick Coleman, Fermilab RESMM’12, February 2012.
Project Overview Ron Ray Mu2e Project Manager Fermilab Sept. 26, 2008 Preliminary Director’s Review of mu2e Fermilab.
Stopped Muon/Pion Measurements Jim Miller, BU May 2012 UW Test Beam Meeting.
Search for Coherent Muon to Electron Conversion: The Mu2e experiment at Fermilab R. Tschirhart Fermilab BEACH 2010, Perugia Italy.
1 fact03 NY June 6 th 2003 Particle physics with intense muon beams A.M. Baldini - INFN Pisa.
Stopped Muon/Pion Measurements Jim Miller, BU May 2012 UW Test Beam Meeting.
Muon Beams for Particle Physics Ajit Kurup Winter Seminar March 2010.
Summary and Status of the Mu2e Experiment at Fermilab 2011 DPF Meeting Craig Group (University of Virginia and Fermilab) …on behalf of the Mu2e collaboration.
Seeing the Subatomic Stephen Miller Saturday Morning Physics October 11, 2003.
F ERMILAB T EST B EAM F ACILITY Aria Soha March 22, 2011.
May William Molzon, UC Irvine Muon Physics at Fermilab 1 Muon Physics at Fermilab Will the physics be important in a global context when the experiment.
Yannis K. Semertzidis Brookhaven National Laboratory MSI-05 KEK, 1-4 March 2005 LFV: Physics Reach LFV Experimental Techniques MECO Experiment at BNL Intensity,
Μ→e search using pulsed muon beam μ -  e - νν nuclear muon capture Muon Decay In Orbit  π - +(A,Z)→(A,Z-1)*, (A,Z-1)* →γ+(A,Z-1), γ→e + e - Prompt.
DISCOVERY OF THE NEUTRON
COMET and DeeMe. Mu-e conversion search at J-PARC COMET Target sensitivity 10 C.L. using aluminum target – SINDRUM II 7x – MEG 2.4x
COMET. μ-e conversion search from muonic aluminium J-PARC pulsed proton beam to produce pulsed muon beam Forbidden in the Standard Model  clue to the.
Lepton Flavor Violation Search via Muon to Electron Conversion W. Molzon, University of California, Irvine B-L International Workshop Berkeley September.
Mu2e and Project X, September 3, 2008 E Prebys Background: Proton Economics in Project X Era* Assume  9mA*1ms = 5.3x10 13 protons/linac “blast”  Main.
1 Beam Extinction and Monitoring at the Upcoming Mu2e Experiment Ryan J. Hooper on behalf of the Mu2e Collaboration DPF 2015 August 5th, 2015.
Physics with the COMET Staging Plan Satoshi MIHARA IPNS, KEK.
 A model of beam line built with G4Beamline (scripting tool for GEANT4)  Simulated performance downstream of the AC Dipole for core of beam using  x.
The MECO Experiment Coherent µ  e Conversion in the Field of a Nucleus P. Yamin, BNL.
M. Garcia-Sciveres July 2002 ATLAS A Proton Collider Detector M. Garcia-Sciveres Lawrence Berkeley National Laboratory.
Neutrino. Game Board FERMILABHAPPENINGSFIRSTSNEUTRINOSDETECTION.
The Mu2e experiment Finding a needle in a trillion haystacks Bertrand Echenard California Institute of Technology FNAL Users' meeting June 2013.
The physics of Mu2e Bertrand Echenard California Institute of Technology Mu2e computing review doc-db XXXXX.
The Mu2e Experiment at Fermilab Mu2e-doc-846-v1 Rob Kutschke, Fermilab April 9, 2010 (NIU Physics Dept. Colloquium)
Mu2e Mu2e Backgrounds and Computing Robert Bernstein 5 March 2015 Mu2e-docdb 5223.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
The Mu2e Experiment at Fermilab Mu2e-doc-800-v1 Rob Kutschke, Fermilab March 9, 2010 (HEP Seminar at U. Minn.)
The Mu2e Experiment at Fermilab Jim Miller Boston University for the Mu2e Collaboration.
The Mu2e Experiment at Fermilab: Giovanni Onorato, Fermilab - INFN Lecce – Universita’ G. Marconi Mu2e Member Institutions: Boston University; Brookhaven.
The Mu2e experiment at Fermilab Finding a needle in a trillion haystacks Bertrand Echenard California Institute of Technology APS Meeting – April 2013.
The Mu2e Experiment at Fermilab Mu2e-doc-1196-v2 Rob Kutschke, Fermilab November 19, 2010 (Cornel Journal Club)
The Mu2e Experiment at Fermilab: Robert K. Kutschke, Fermilab Within the Standard Model, muons decay in a way that almost perfectly conserves lepton family.
Minerva Test Beam 2 Status Geoff Savage for the Test Beam 2 Team March 23, /23/2015AEM - Minerva Test Beam 2 Status1.
The Mu2e Experiment A search for charged lepton flavor violation at FNAL For the Mu2e Collaboration Kevin Lynch Boston University 2010 Fermilab Users'
New cLFV search experiments using the mu-e conversion process Satoshi MIHARA KEK, Japan.
Straw Tracker Crystal Calorimeter Stopping Target Robert K. Kutschke [1], Fermilab The Mu2e experiment at Fermilab is in the midst of its R&D and approval.
The Mu2e Experiment at Fermilab Mu2e-doc-3227-v4
A New Sensitive Search for Muon to Electron Conversion Mu2e Experiment at Fermilab Mu2e Collaboration: Boston U, BNL, UC Berkeley & LBNL, UC Irvine, CUNY,
Tracker for the mu2e Experiment at Fermilab Aseet Mukherjee Bob Wagner.
The New CHOD detector for the NA62 experiment at CERN S
Mu2e : 10 Minutes in Questions
Search for CLFV at COMET experiment muon to electron conversion
The COMET Experiment Ajit Kurup, Imperial College London, on behalf of the COMET Collaboration. ABSTRACT The COherent Muon to Electron Transition (COMET)
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
The Mu2e experiment at Fermilab
COherent Muon to Electron Transition (COMET)
What is μ-e Conversion ? μ μ-+(A,Z)→e-+(A,Z) muon decay in orbit
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Presentation transcript:

Giovanni Onorato Fermilab University of Rome “Guglielmo Marconi” INFN Lecce Mu2e general presentation

/ 156 / 28 / Particle physics frontiers - Neutrino experiments (NOvA, LBNE, MINOS, MINERvA, and others… ) - Precision measurements (g-2) - Rare decays (Mu2e) Mu2e collaboration

/ 156 / 28 / The lepton flavor violation Neutrinos have mass, so in the SM we can have Rate < (unmeasurably low) In new physics models one can have or in presence of a nucleus… Experiments:Mu2e, SINDRUM II, TRIUMF, COMMET, and others… Rate ~

/ 156 / 28 / Present measurements

/ 156 / 28 / Mu2e achievements

/ 156 / 28 / Experimental setup 1 Proton beam hits production target in Production Solenoid. Pions captured and accelerated towards Transport Solenoid by graded field. Pions decay to muons.

/ 156 / 28 / Experimental setup II Transport solenoid performs sign and momentum selection. Eliminates high energy negative particles, positive particles and line-of- sight neutrals. Muons captured in stopping target. Conversion electron trajectory measured in tracker, validated in calorimeter. Cosmic Ray Veto surrounds Detector Solenoid.

/ 156 / 28 / Dominant background

/ 156 / 28 / Other background sources - Radiative muon/pion capture - Photon produced that can convert asymmetrically - Beam electrons can scatter in target - Muon/pion decay in flight - Antiprotons and other late arriving particles - Cosmic-ray induced electrons - Protons - Neutrons - Photons from Nuclear capture None of them produce a sharp peak at 105 MeV: they need to be well known and controlled. Work is going on on this

/ 156 / 28 / Detectors: the T-Tracker 18 stations + Stiffening rings at ends 12 panels, at 30° rotations, form a station 30° stereo angles give 400m resolution along wire Straw termination and readout at r>70cm

/ 156 / 28 / T-Tracker: straws structure 5mm straws Gaps between straws Double layer

/ 156 / 28 / Alt. ITracker (from INFN Lecce)

/ 156 / 28 / The calorimeter (from INFN Frascati/Pisa)

/ 156 / 28 / Location

/ 156 / 28 / Time schedule