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WG4 Summary -Intense Muon Physics- Conveners

WG4 Summary -Intense Muon Physics- Conveners Y. Semertzdis (BNL), M. Grassi (Pisa), K. Ishida (RIKEN) summary-1 for muon applications by K. Ishida. Muon Physics (the Standard Model and beyond) LFV g-2 and EDM Life time Michel parameters Muon Applications (Physics with muons)

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WG4 Summary -Intense Muon Physics- Conveners

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  1. WG4 Summary -Intense Muon Physics- Conveners Y. Semertzdis (BNL), M. Grassi (Pisa), K. Ishida (RIKEN) summary-1 for muon applications by K. Ishida

  2. Muon Physics (the Standard Model and beyond) LFV g-2 and EDM Life time Michel parameters Muon Applications (Physics with muons) m- : heavy electron muonic atom, nuclear capture muonic atoms and molecules muon catalyzed fusion m+ : light proton mSR (muon spin rotation/relaxation/resonance) muonium (atomic physics) muon as beam radiography summary by Y. Semertzdis summary by K. Ishida

  3. Muon for unstable nuclear physics P. Strasser X-RAY SPECTROSCOPY of MUONIC ATOMS ! 􀂷 Powerful tool to probe the NUCLEAR CHARGE DISTRIBUTION. How to produce exotic mA* atoms of unstable nuclei?

  4. Muon catalyzed fusion K. Ishida rich in few body physics problems muon catalyzing more than 120 fusions progress and plans for increasing mCF am reactivation process high density, high temperature target control of molecule states

  5. mSR (muon spin rotation/relaxation/resonance) Y. J. Uemura E. Morenzoni in plenary materials science with muons example: • (muon spin relaxation) as probe of superconducting (s.c.) pair density classification of s.c. systems and study of s.c. mechanism

  6. Low energy (or ultra slow) muon beam E. Morenzoni in plenary Y. Matsuda Cryogenic moderator method (PSI) surface science thin layer/multilayers depth profile of field penetration beam intensity rapid progress at RIKEN-RAL 1000/s x 7 expected at PSI this year Laser resonant ionization method (KEK)

  7. Radiograpy with high energy muon beam K. Nagamne Energy loss and scattering angle vs thickness and Z-dep. TeV Cosmic ray probing a volcano 400MeV 1m water Compact muon source for advanced muon radiography nuclear inspection, industrial machinery …

  8. For more muon beams H. Miyadera Axial focusing surface muon beam transportation, 1.3sr Axisymmetric m-e separator electron positron muon

  9. Future muon beams for muon science MLF (Materials and Life Science) at J-PARC 3GeV MLF Muon Facility has started construction To be realized in 4 years Y. Miyake Muon Facility 3GeV 333A Surface Muon Ports 107/s (4MeV) DecayPorts 107/s (10-50MeV) Intense Surface & Negative muon port SlowPorts 104-5/s (eV-keV) J-PARC

  10. Muon SciencePhase 1 Decay-Surface Muon Port Surface Muon Port Muon SciencePhase 2Curved Solenoid Port For Ultra Slow Muon & Negative Muon Beams Beam shift along path calculated by Ishida Muon SciencePhase 2’High Momemtum Decay Muon Port

  11. Muon Facility for Particle Physics at J-PARC 50GeV Fast extraction facility for muon physics : me conversion, edm, g-2 anti-proton phyiscs : antimatter etc aim at 1011~1012/s with PRISM for PRIME, PRISM-II for g-2 and edm LOIs to J-PARC organization of global collaboration A. Sato J-PARC 50GeV

  12. Summary of muon applications part Good progress in wide range of muon science Steady increase (x10 or more) is expected in muon beam intensity of various characters (slow muon, pulsed muon) Several orders magnitude increase of muon intensity aimed at neutrino-factory would have strong impact on muon application sciences (needs matching beam properties, beam slot, facilities) and also could open a new field of applications..

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