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.

Slides:



Advertisements
Similar presentations
Flavor Beyond the Standard Model Zurab Tavartkiladze, Gela Devidze Tbilisi State University Volkswagen meeting 14, 15 March 2013, Tbilisi.
Advertisements

LBL Comet-Mu2E Workshop January 24, 2009 Mu-e Conversion Backgrounds and Sensitivities– from proposal to measurement Doug Bryman "Wishing does not make.
Yingchuan Li Weak Mixing Angle and EIC INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider Energies Sep. 17th 2010.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
The COherent Muon to Electron Transition (COMET) Experiment
K. Kumar, W. Marciano, Y. Li Electroweak physics at EIC - Summary of week 7 INT Workshop on Pertubative and Non-Pertubative Aspects of QCD at Collider.
The MINOS Experiment Andy Blake Cambridge University.
The Mu2e Experiment at Fermilab Jim Miller Boston University for the Mu2e Collaboration June 6, 2008.
1 Overview and Challenges for Upgrades: Muon-Electron Conversion at FNAL R. Bernstein Fermilab for the Mu2e Collaboration R. Bernstein Fermilab for the.
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.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
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.
Search for Coherent Muon to Electron Conversion: The Mu2e experiment at Fermilab R. Tschirhart Fermilab BEACH 2010, Perugia Italy.
Yannis K. Semertzidis Brookhaven National Laboratory NuFact04 Osaka, 26 July- 1 Aug LFV: Why is it important? LFV Experimental Techniques MECO Experiment.
1 fact03 NY June 6 th 2003 Particle physics with intense muon beams A.M. Baldini - INFN Pisa.
 N-eN Rare Process M. Aoki, Osaka University MuSAC-2009, Tokai, 2010/3/10-11.
Muon Beams for Particle Physics Ajit Kurup Winter Seminar March 2010.
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,
Slow extraction septa requirements for Rare Symmetry Violating Processes (RSVP) experiments at BNL K.A. Brown Collider Accelerator Department, BNL.
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.
G-2, EDM, COMET muon particle physics programmes at J-PARC Mu_01 Satoshi MIHARA IPNS, KEK FKPPL-FJPPL workshop, Yonesei Univ.
Douglas Bryman University of British Columbia Seeking New Physics with Rare Decays Early Adventures at TRIUMF and Future Prospects JMP Retirement Symposium.
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.
Giovanni Onorato Fermilab University of Rome “Guglielmo Marconi” INFN Lecce Mu2e general presentation.
Douglas Bryman University of British Columbia APS May 3, 2011.
1 Beam Extinction and Monitoring at the Upcoming Mu2e Experiment Ryan J. Hooper on behalf of the Mu2e Collaboration DPF 2015 August 5th, 2015.
Medium baseline neutrino oscillation searches Andrew Bazarko, Princeton University Les Houches, 20 June 2001 LSND: MeVdecay at rest MeVdecay in flight.
 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.
Parametrisation of PRISM Ring and Design Options J. Pasternak Imperial College London/RAL STFC PRISM-FFAG Task Force phone meeting,
Eric Prebys Fermilab For the Mu2e Collaboration November 16, 2010.
Search for Lepton Flavor Violation (LFV) in e+e– interaction (review of experimental results) M.N. Achasov International Workshop on e+e– collisions from.
Steering Group Meeting 10:30 – 12:30 am CDT Monday, July 23, 2007 Y2K.
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)
Production Solenoid Detector Solenoid Transport Solenoid Calorimeter Tracker Production Target Proton Beam The Mu2e Experiment at Fermilab: A Search for.
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.
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.
The Mu2e Experiment at Fermilab Mu2e-doc-3227-v4
Search for Anomalous Production of Multi-lepton Events at CDF Alon Attal Outline  Motivation  R p V SUSY  CDF & lepton detection  Analysis  Results.
A New Sensitive Search for Muon to Electron Conversion Mu2e Experiment at Fermilab Mu2e Collaboration: Boston U, BNL, UC Berkeley & LBNL, UC Irvine, CUNY,
Mu2e : 10 Minutes in Questions
Search for CLFV at COMET experiment muon to electron conversion
A New Charged Lepton Flavor Violation Experiment: Muon-Electron Conversion at FNAL.
POFPA 17/3/06 A. Ceccucci K & B: Theory vs. Experiments
Cecilia Voena INFN Roma on behalf of the MEG collaboration
The COMET Experiment Ajit Kurup, Imperial College London, on behalf of the COMET Collaboration. ABSTRACT The COherent Muon to Electron Transition (COMET)
CSN1 Presentation December 3, 2012 Ron Ray Mu2e Project Manager
The Mu2e experiment at Fermilab
Prospects for CLFV experiments
Particle Physics: Status and Perspectives Part 8: The Precision Frontier Manfred Jeitler SS 2018.
COherent Muon to Electron Transition (COMET)
What is μ-e Conversion ? μ μ-+(A,Z)→e-+(A,Z) muon decay in orbit
Decay Angular Measurement in the MEG Experiment
Presentation transcript:

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.

The Frontiers of Particle Physics 8/2011C. Group - Mu2e Summary DPF Meeting2 Mu2e

The Intensity Frontier! One can probe the properties of the universe by looking for extremely rare processes Complementary alternative to using higher energies The medium-term future of accelerator-based particle physics on US soil is the intensity frontier : – Neutrino experiments (NOvA, LBNE, MINOS, MINERvA, and others… ) – Precision measurements (g-2) – Rare decays (Mu2e, MEG, COMET, and others) 8/2011C. Group - Mu2e Summary DPF Meeting3

Charged Lepton Flavor Violation (CLFV) 8/2011C. Group - Mu2e Summary DPF Meeting4 Neutrinos have mass!  individual lepton numbers are not conserved! Therefore, Lepton Flavor Violation occurs in Charged Leptons! Neutrinos have mass!  individual lepton numbers are not conserved! Therefore, Lepton Flavor Violation occurs in Charged Leptons! NO PHYSICS BACKGROUND! Observation is unambiguous sign of new physics! NO PHYSICS BACKGROUND! Observation is unambiguous sign of new physics!

Searching for CLFV 8/2011C. Group - Mu2e Summary DPF Meeting5 μ  eγ Can look for muon decaying into an electron plus a photon: Experiments : MEGA, MEG, and others…

Searching for CLFV 8/2011C. Group - Mu2e Summary DPF Meeting6 μ+N  e+N In the presence of a nucleus (N): The electron is mono-energetic in CM frame! Experiments:Mu2e, SINDRUM II, TRIUMF, COMET, and others…

Mu2e Goal: Search for – Measure ratio: – With sensitivity to R at 90% C.L. of 6*  4 orders of magnitude better than current limits  Need more than stopped muons! *10 20 protons on target (2 year run – 2x10 7 s)  Need to keep background small and well understood 8/2011C. Group - Mu2e Summary DPF Meeting7 Experiment with preliminary approval that is proposed to begin data taking in 2018 at Fermilab.

Experimental Signature 8/2011C. Group - Mu2e Summary DPF Meeting 8 A single monoenergetic electron If N = Al, E e = 105. MeV (Electron E depends on Z) Nucleus coherently recoils off outgoing electron, no breakup A single monoenergetic electron If N = Al, E e = 105. MeV (Electron E depends on Z) Nucleus coherently recoils off outgoing electron, no breakup e-e- --

Background Processes Signal is a single 105 MeV e-. Many possible sources of background events: – Muon decay in Coulomb orbit (DIO) – 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 8/2011C. Group - Mu2e Summary DPF Meeting9 These can all be controlled and none produce a sharp peak at 105 MeV!

History of CLFV Searches 8/2011C. Group - Mu2e Summary DPF Meeting10

History of CLFV Searches 8/2011C. Group - Mu2e Summary DPF Meeting11 New MEG result: 2.4x arXiv: July 2011

CLFV from SUSY 8/2011C. Group - Mu2e Summary DPF Meeting12 In Mu2e, a signal of Terascale physics at LHC implies: 40 signal events ~ 0.2 background events ~ ~ Access to SUSY through loops.

Other “new physics” also provide Mu2e signal 8/2011C. Group - Mu2e Summary DPF Meeting13 Marciano, Mori, and Roney, Ann. Rev. Nucl. Sci. 58

C. Group - Mu2e Summary DPF Meeting CLFV in  + → e +  and  - N → e - N  << 1 magnetic moment type operator  → e  rate ~300X  N → eN rate  >> 1 four-fermion interaction  N → eN >>  → e  rate Model independent effective CLFV Lagrangian Mass scales probed ~10,000 times that probed directly by LHC 8/ Loops Contact Interactions Loops Contact

Constraints on new physics Mu2e Complementarity between Lepton Flavor Violation (LFV) and LHC experiments Complementarity between Lepton Flavor Violation (LFV) and LHC experiments Minimal Flavor Violation(CKM) Neutrino-Matrix Like (PMNS) Can distinguish between PMNS and MFV Can distinguish between PMNS and MFV Current limits L. Calibbi, A. Faccia, A. Masiero, S. Vempati hep-ph/ /2011C. Group - Mu2e Summary DPF Meeting15

Constraints on new physics 8/2011C. Group - Mu2e Summary DPF Meeting16 Goal

Mu2e Beyond the LHC 8/2011C. Group - Mu2e Summary DPF Meeting17 Provides information about flavor structure of new physics even if it is not easily accessible at the LHC. A null result at the proposed sensitivity will severely constrain new physics models. CLFV is predicted at observable rates for Mu2e in many models of new physics. Mu2e can probe mass scales up to 10 4 TeV, far beyond the direct reach of the LHC.

The Mu2e Experiment 8/2011C. Group - Mu2e Summary DPF Meeting18 Proton Beam Proton beam hits production target in Production Solenoid. Pions captured and accelerated towards Transport Solenoid by graded field. Pions decay to muons. (for sense of scale) 1)

The Mu2e Experiment 8/2011C. Group - Mu2e Summary DPF Meeting19 Proton Beam Proton beam hits production target in Production Solenoid. Pions captured and accelerated towards Transport Solenoid by graded field. Pions decay to muons. (for sense of scale) 1) Courtesy of Symmetry Magezine

The Mu2e Experiment 8/2011C. Group - Mu2e Summary DPF Meeting20 Proton Beam Transport solenoid performs sign and momentum selection. Eliminates high energy negative particles, positive particles and line-of-sight neutrals. 2)

The Mu2e Experiment 8/2011C. Group - Mu2e Summary DPF Meeting21 Proton Beam Muons stop in target and decay. Conversion electron trajectory measured in tracker, validated in calorimeter. Cosmic Ray Veto surrounds Detector Solenoid. 3)

8/2011C. Group - Mu2e Summary DPF Meeting22 Sensitivity Goal X10000 improvement over current best limit! How: Improved efficiency for producing and stopping muons Production target in gradient field* Mu2e will stop 50 billion muons per second! Expect to stop 21 muons per 10,000 proton on target. Reduced backgrounds and detector occupancy due to pulsed beam Single event sensitivity! <0.2 bkg events expected in 2-year run * Djilkibaev, Lobashev et. al.

4 Orders-of-Magnitude? We have the best accelerator setup in the world for this measurement! Ideal pulse spacing… 8/2011C. Group - Mu2e Summary DPF Meeting23 Bunch structure Extinction level of between bunches is crucial! (Removes ‘prompt’ backgrounds!) (μ lifetime in 1s orbit of AL ~864 ns)

4 Orders-of-Magnitude?  Straw tracker designed such that no acceptance for lower-energy electrons from muon decay in orbit. 8/2011C. Group - Mu2e Summary DPF Meeting24

4 Orders-of-Magnitude? 8/2011C. Group - Mu2e Summary DPF Meeting25 Long tail due to nuclear recoil Conversion momentum shifted due to material interactions

Mu2e Schedule C. Group - Mu2e Summary DPF Meeting268/2011 Design Phase Solenoid Design Solenoid Fabrication Detector Hall Construction Detector Construction

The Mu2e Collaboration Boston University Brookhaven National Laboratory Cal Tech University of California, Berkeley University of California, Irvine City University of New York Duke University Fermilab University of Houston University of Illinois, Urbana-Champaign Boston University Brookhaven National Laboratory Cal Tech University of California, Berkeley University of California, Irvine City University of New York Duke University Fermilab University of Houston University of Illinois, Urbana-Champaign Institute for Nuclear Research, Moscow JINR, Dubna, Russia Lawrence Berkeley National Laboratory Los Alamos National Laboratory Northwestern University INFN Frascati INFN Pisa, Università di Pisa, Pisa, Italy University of Massachusetts Institute for Nuclear Research, Moscow JINR, Dubna, Russia Lawrence Berkeley National Laboratory Los Alamos National Laboratory Northwestern University INFN Frascati INFN Pisa, Università di Pisa, Pisa, Italy University of Massachusetts INFN Lecce, Università del Salento, Italy Rice University Syracuse University University of Virginia College of William and Mary University of Washington, Seattle INFN Lecce, Università del Salento, Italy Rice University Syracuse University University of Virginia College of William and Mary University of Washington, Seattle ~120 collaborators ~120 collaborators 8/2011C. Group - Mu2e Summary DPF Meeting27

Summary The intensity frontier and flavor physics may well reveal a sign of exotic physics! Mu2e will improve sensitivity by 4 orders-of- magnitude relative to past CLFV searches. Mu2e will provide complementary information relative to the LHC and is sensitive to mass scales many orders of magnitude higher than can be directly probed at colliders. 8/2011C. Group - Mu2e Summary DPF Meeting28

Backup 8/2011C. Group - Mu2e Summary DPF Meeting29

CDR 8/2011C. Group - Mu2e Summary DPF Meeting30

Mu2e Review Status Mu2e received mission-need approval from DOE in November From our Mission Need Statement: – “A muon-to-electron conversion experiment at Fermilab could provide an advance in experimental sensitivity of four orders of magnitude.” We have a complete set of requirements designed to meet this goal:  Describes what each major system component must achieve We have a conceptual design that we believe satisfies these requirements. Mu2e had a successful Independent Design Review on May 3 rd and 4 th Two more reviews later this Summer… Goal: Approved conceptual design by end of 2011 C. Group - Mu2e Summary DPF Meeting318/2011

Possible Scenarios We see something the first year! – Change target to better constrain the new physics rule out some backgrounds. See something with two years of data: – Plan for intensity upgrade – New targets… Don’t see anything: – Intensity upgrade to Project X for sensitivity improvement of two additional orders-of-magnitude. 8/2011C. Group - Mu2e Summary DPF Meeting32

CLFV and Tau Decays 33 τ processes also suppressed in Standard Model but less: τ processes also suppressed in Standard Model but less: SM ~ SM ~ Lee, Shrock Phys.Rev.D16:1444,1977 Pham, hep-ph/ Good News: Beyond SM rates are several orders of magnitude larger than in associated muon decays Good News: Beyond SM rates are several orders of magnitude larger than in associated muon decays Bad News: τ ’s hard to produce: ~10 10 τ /yr vs ~10 11 μ /sec in fixed-target experiments (Mu2e/COMET) Bad News: τ ’s hard to produce: ~10 10 τ /yr vs ~10 11 μ /sec in fixed-target experiments (Mu2e/COMET) Smaler GIM Cancellations because of large τ mass Smaler GIM Cancellations because of large τ mass also e → τ at electron-ion collider? M. GonderingerM. Gonderinger, M. Ramsey-Musolf, arXiv: v1lf, arXiv: also e → τ at electron-ion collider? M. GonderingerM. Gonderinger, M. Ramsey-Musolf, arXiv: v1lf, arXiv: /2011 C. Group - Mu2e Summary DPF Meeting33

34 R. Bernstein, FNAL Mu2e Pittsburgh Feb 2011 Supersymmetry in Tau LFV Neutrino mass via the see--saw mechanism, analysis is performed in an SO(10) framework L. Calibbi, A. Faccia, A. Masiero, S. Vempati hep-ph/ Neutrino-Matrix Like (PMNS) Minimal Flavor Violation(CKM) 8/2011C. Group - Mu2e Summary DPF Meeting