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

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Presentation transcript:

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)  - : heavy electron muonic atom, nuclear capture muonic atoms and molecules muon catalyzed fusion  + : light proton  SR (muon spin rotation/relaxation/resonance) muonium (atomic physics) muon as beam radiography summary by Y. Semertzdis summary by K. Ishida

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

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

 SR (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

Cryogenic moderator method (PSI) Laser resonant ionization method (KEK) Low energy (or ultra slow) muon beam E. Morenzoni in plenary Y. Matsuda 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

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

Proton CurrentTarget Thickness Muon Intensity  + / pulse Dai Omega 500MeV 5  A 4mm 4 x 10 5  + / s 2 x 10 4 KEK-MSL I 500MeV 5  A 30mm 2.5 x 10 4  + / s 1.3 x 10 3 RAL 800MeV 200  A 10mm ~10 6  + / s ~2 x 10 4 electron positron muon Axisymmetric  -e separator Axial focusing surface muon beam transportation, 1.3sr For more muon beams H. Miyadera

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 Muon Facility 3GeV 333  A Surface Muon  Ports 10 7 /s (4MeV) Decay       Ports 10 7 /s (10-50MeV) Intense Surface & Negative muon port Slow      Ports /s (eV-keV) J-PARC Y. Miyake

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

Muon Facility for Particle Physics at J-PARC 50GeV Fast extraction facility for muon physics :  e conversion, edm, g-2 anti-proton phyiscs : antimatter etc aim at ~10 12 /s with PRISM for PRIME, PRISM-II for g-2 and edm LOIs to J-PARC organization of global collaboration J-PARC 50GeV A. Sato

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..