WG4 Summary -Intense Muon Physics-

ConvenersY Semertzdis (BNL) M Grassi (Pisa) K Ishida (RIKEN)

summary-1 for muon applicationsby K Ishida

Muon Physics (the Standard Model and beyond)LFV

g-2 and EDMLife timeMichel parameters

Muon Applications (Physics with muons)- heavy electron

muonic atom nuclear capturemuonic atoms and moleculesmuon catalyzed fusion

+ light protonSR (muon spin rotationrelaxationresonance)muonium (atomic physics)

muon as beamradiography

summary by Y Semertzdis

summary by K Ishida

Muon for unstable nuclear physics

X-RAY SPECTROSCOPY of MUONIC ATOMS

1048759 Powerful tool to probe the NUCLEAR

CHARGE DISTRIBUTION

How to produce exotic A atoms of unstable nuclei

P Strasser

tmicro

dmicro

microdtmicro

n

micro

dtmicroformation

nuclearfusion

effective stickings=(1-R)s0

176MeV x Ynenergy output

injectedmuon

d

KKX-ray

14MeVneutron

3Hemicrotransfer toHe

rich in few body physics problemsmuon catalyzing more than 120 fusionsprogress and plans for increasing CF

reactivation processhigh density high temperature targetcontrol of molecule states

Muon catalyzed fusionK Ishida

SR (muon spin rotationrelaxationresonance)

Y J UemuraE Morenzoni in plenary

materials science with muons

example(muon spin relaxation) as probe of superconducting (sc) pair densityclassification of sc systems andstudy of sc mechanism

Cryogenic moderator method (PSI)

Laser resonant ionization method (KEK)

Low energy (or ultra slow) muon beam

E Morenzoni in plenaryY Matsuda

surface sciencethin layermultilayersdepth profile of field penetration

beam intensityrapid progress at RIKEN-RAL1000s x 7 expected at PSI this year

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

Muon Physics (the Standard Model and beyond)LFV

g-2 and EDMLife timeMichel parameters

Muon Applications (Physics with muons)- heavy electron

muonic atom nuclear capturemuonic atoms and moleculesmuon catalyzed fusion

+ light protonSR (muon spin rotationrelaxationresonance)muonium (atomic physics)

muon as beamradiography

summary by Y Semertzdis

summary by K Ishida

Muon for unstable nuclear physics

X-RAY SPECTROSCOPY of MUONIC ATOMS

1048759 Powerful tool to probe the NUCLEAR

CHARGE DISTRIBUTION

How to produce exotic A atoms of unstable nuclei

P Strasser

tmicro

dmicro

microdtmicro

n

micro

dtmicroformation

nuclearfusion

effective stickings=(1-R)s0

176MeV x Ynenergy output

injectedmuon

d

KKX-ray

14MeVneutron

3Hemicrotransfer toHe

rich in few body physics problemsmuon catalyzing more than 120 fusionsprogress and plans for increasing CF

reactivation processhigh density high temperature targetcontrol of molecule states

Muon catalyzed fusionK Ishida

SR (muon spin rotationrelaxationresonance)

Y J UemuraE Morenzoni in plenary

materials science with muons

example(muon spin relaxation) as probe of superconducting (sc) pair densityclassification of sc systems andstudy of sc mechanism

Cryogenic moderator method (PSI)

Laser resonant ionization method (KEK)

Low energy (or ultra slow) muon beam

E Morenzoni in plenaryY Matsuda

surface sciencethin layermultilayersdepth profile of field penetration

beam intensityrapid progress at RIKEN-RAL1000s x 7 expected at PSI this year

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

Muon for unstable nuclear physics

X-RAY SPECTROSCOPY of MUONIC ATOMS

1048759 Powerful tool to probe the NUCLEAR

CHARGE DISTRIBUTION

How to produce exotic A atoms of unstable nuclei

P Strasser

tmicro

dmicro

microdtmicro

n

micro

dtmicroformation

nuclearfusion

effective stickings=(1-R)s0

176MeV x Ynenergy output

injectedmuon

d

KKX-ray

14MeVneutron

3Hemicrotransfer toHe

rich in few body physics problemsmuon catalyzing more than 120 fusionsprogress and plans for increasing CF

reactivation processhigh density high temperature targetcontrol of molecule states

Muon catalyzed fusionK Ishida

SR (muon spin rotationrelaxationresonance)

Y J UemuraE Morenzoni in plenary

materials science with muons

example(muon spin relaxation) as probe of superconducting (sc) pair densityclassification of sc systems andstudy of sc mechanism

Cryogenic moderator method (PSI)

Laser resonant ionization method (KEK)

Low energy (or ultra slow) muon beam

E Morenzoni in plenaryY Matsuda

surface sciencethin layermultilayersdepth profile of field penetration

beam intensityrapid progress at RIKEN-RAL1000s x 7 expected at PSI this year

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

tmicro

dmicro

microdtmicro

n

micro

dtmicroformation

nuclearfusion

effective stickings=(1-R)s0

176MeV x Ynenergy output

injectedmuon

d

KKX-ray

14MeVneutron

3Hemicrotransfer toHe

rich in few body physics problemsmuon catalyzing more than 120 fusionsprogress and plans for increasing CF

reactivation processhigh density high temperature targetcontrol of molecule states

Muon catalyzed fusionK Ishida

SR (muon spin rotationrelaxationresonance)

Y J UemuraE Morenzoni in plenary

materials science with muons

example(muon spin relaxation) as probe of superconducting (sc) pair densityclassification of sc systems andstudy of sc mechanism

Cryogenic moderator method (PSI)

Laser resonant ionization method (KEK)

Low energy (or ultra slow) muon beam

E Morenzoni in plenaryY Matsuda

surface sciencethin layermultilayersdepth profile of field penetration

beam intensityrapid progress at RIKEN-RAL1000s x 7 expected at PSI this year

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

SR (muon spin rotationrelaxationresonance)

Y J UemuraE Morenzoni in plenary

materials science with muons

example(muon spin relaxation) as probe of superconducting (sc) pair densityclassification of sc systems andstudy of sc mechanism

Cryogenic moderator method (PSI)

Laser resonant ionization method (KEK)

Low energy (or ultra slow) muon beam

E Morenzoni in plenaryY Matsuda

surface sciencethin layermultilayersdepth profile of field penetration

beam intensityrapid progress at RIKEN-RAL1000s x 7 expected at PSI this year

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

Cryogenic moderator method (PSI)

Laser resonant ionization method (KEK)

Low energy (or ultra slow) muon beam

E Morenzoni in plenaryY Matsuda

surface sciencethin layermultilayersdepth profile of field penetration

beam intensityrapid progress at RIKEN-RAL1000s x 7 expected at PSI this year

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

TeV Cosmic ray probinga volcano

Compact muon source for advanced muon radiography nuclear inspection industrial machinery hellip

Energy loss and scattering anglevs thickness and Z-dep

Radiograpy with high energy muon beam K Nagamne

400MeV

1m water

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

Proton Current Target Thickness Muon Intensity + pulse

Dai Omega 500MeV 5 A 4mm 4 x 105 + s 2 x 104

KEK-MSL I 500MeV 5 A 30mm 25 x 104 + s 13 x 103

RAL 800MeV 200A 10mm ~106 + s ~2 x 104

-07

-06

-05

-04

-03

-02

-01

0

01

-500E-07

-450E-07

-400E-07

-350E-07

-300E-07

-250E-07

-200E-07

-150E-07

-100E-07

-500E-08

000E+00

Separator 40kV

Separator off

electronpositron

muon

Axisymmetric -e separator

Axial focusing surface muon beam transportation 13sr

For more muon beamsH Miyadera

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

Future muon beams for muon science

MLF (Materials and Life Science) at J-PARC 3GeVMLF Muon Facility has started constructionTo be realized in 4 years

Muon Facility 3GeV 333A

Surface Muon Ports 107s (4MeV)

Decay 　 Ports 107s (10-50MeV)

Intense Surface amp Negative muon port

Slow 　 Ports 104-5s (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 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12

Muon Science Phase 1 Decay-Surface Muon Port Surface Muon Port

Beam shift along path calculated by Ishida

Muon Science Phase 2Curved Solenoid Port For Ultra Slow Muon amp Negative Muon Beams

Muon Science Phase 2rsquo 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 etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

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Muon Facility for Particle Physics at J-PARC 50GeV

Fast extraction facility for muon physics e conversion edm g-2 anti-proton phyiscs antimatter etcaim at 1011~1012s with PRISM for PRIME PRISM-II for g-2 and edmLOIs to J-PARCorganization 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 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

• Slide 1
• Slide 2
• Slide 3
• Slide 4
• Slide 5
• Slide 6
• Slide 7
• Slide 8
• Slide 9
• Slide 10
• Slide 11
• Slide 12