precision particle physics at psi - university of tokyo€¦ · precision particle physics at psi...
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Klaus Kirch 1 Tokyo, Feb 18, 2016
Precision particle physics at PSI K.Kirch, ETH Zurich – PSI Villigen, Switzerland
Using highest intensities of
pions, muons and UCN for
• Precision measurements of
Standard Model parameters
• Searches for physics beyond
the Standard Model
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Klaus Kirch 2 Tokyo, Feb 18, 2016
The Standard Model of Particle Physics
is extremely successful … (with some issues concerning neutrino masses,
muon g-2, B-decays, …)
… but does not explain Gravity, Dark matter
Dark energy
3 families
QCD theta term
Values of particle masses and couplings
Baryon Asymmetry of the Universe
Conservation of baryon and charged lepton number
…
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Klaus Kirch 3 Tokyo, Feb 18, 2016
PSI Laboratory for Particle Physics Discovery Physics at
high and low energies
Precision measurements
(MuLan, CREMA, MuCap,
MuSun, MUSE ..) and
searches for new physics
(MEG, nEDM, Mu3e,
n2EDM, ...) at PSI
At LHC:
Participation and key
contributions to CMS
(Si-pixel R&D and data
analysis, e.g. B-mm at PSI)
Particle phenomenology
Collaborations with all Swiss universities
many universities and
institutions world-wide
Outreach and Spin-off Detectors (pixel, gas and
scintillation) for particle
physics; n, mSR, x-rays
Chip design, electronics and
software for PSI and world-
wide, e.g. DRS-4, elog, Midas, ...
Irradiation using p, p, m, e
Zuoz schools (2016: 23rd!)
PSI20xy workshop: PSI2016
LTP-Groups
Theory
High Energy Physics
Muon Physics
Ultacold Neutrons
Electronics and
Measurement Systems
Detectors
Applied Particle Physics
and Irradiations
Academic links to universities:
common professorships
and teaching
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Klaus Kirch 4 Tokyo, Feb 18, 2016
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Klaus Kirch 5 Tokyo, Feb 18, 2016
The Heart of HIPA: The Ring Cyclotron
• at time of construction a new
concept: separated sector
Ring cyclotron [H.Willax et al.]
• 8 magnets (280t),
4 accelerating resonators
(50MHz), 1 Flattop (150MHz),
15m
• losses at extraction 200W
• red. losses by increasing RF
voltage was main upgrade
path
[losses (turn number)3, W.Joho]
150MHz resonator 50MHz resonator
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Klaus Kirch 6 Tokyo, Feb 18, 2016
History of maximum beampower
milestones:
• new injector
cyclotron (‘84)
• upgrading Ring
RF power
• replacing Ring
cavities
• new ECR
source
Originally
planned: 100mA
today: 2.400mA
[routine: 2.200mA]
Courtesy: M. Seidel
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Klaus Kirch 7 Tokyo, Feb 18, 2016
High Intensity Proton Accelerator
– the international context
Ebeam [GeV]
1MW
10MW
100kW
Courtesy: M. Seidel
1 10
1
Iavg
[m
A]
10
0.1
PSI HIPA serves three communities
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Klaus Kirch 8 Tokyo, Feb 18, 2016
The intensity frontier at PSI: p, m, UCN
nEDM
CREMA: mp / md / mHe laser spectroscopy
MuLan/MuCap
MEG Mu3e
PEN
PIF
nTRV The most powerful
proton beam to targets:
590 MeV x 2.4 mA = 1.4 MW
The highest intensity
pion and muon beams, e.g.,
up to a few 108m+/s at 28 MeV/c The new high intensity
ultracold neutron source
Swiss national laboratory with strong international collaborations
Precision experiments with the lightest unstable particles of their kind
MuSun
MUSE
pHe
Feasibility study for
HI muon beam with
1010m+/s below 30 MeV/c
AlCap MuX muCool
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Klaus Kirch 9 Tokyo, Feb 18, 2016
Precision physics I: Ordinary muon decay
…
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Klaus Kirch 10 Tokyo, Feb 18, 2016
The Weak coupling constant GF
MuLan: The most precise measurement of any lifetime:
Fundamental electro-weak parameters of the Standard Model
a GF mZ
0.00037ppm 4.1 0.5 ppm 23ppm
MuLan: Illinois, Kentucky, Boston, J.Madison, Regis, Wesleyan, PSI,KVI
D.M. Webber et al., PRL 106(2011)041803
www.npl.washington.edu/muon/
V. Tishchenko et al., PRD 87(2013)052003
t = 2 196 980.3 ± 2.2 ps (1.0 ppm)
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Klaus Kirch 11 Tokyo, Feb 18, 2016
The most precise value of the
proton charge radius via a
measurement of the Lambshift
in muonic hydrogen
Bound state QED
R. Pohl et al., Nature 466 (2010) 213
A. Antognini et al., Science 339 (2013) 417
www.psi.ch/muonic-atoms
rp=0.84087(39) fm
Precision physics II
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Klaus Kirch 12 Tokyo, Feb 18, 2016
Charge radii of the
proton and the
deuteron extracted from
precision measurement
of the muonic atom
2S-2P Lambshift.
Also measured:
muonic He-3, He-4.
Next spectroscopy:
- muonic p, He-3 HFS
- muonic radium
- Muonium 1S-2S
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Klaus Kirch 13 Tokyo, Feb 18, 2016
The mp 2S-2P Lambshift experiment
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Klaus Kirch 14 Tokyo, Feb 18, 2016
Search for new physics
For example:
Search for meg
g
m- e-
0~
m~
e~
High Energy High Intensity
direct production of new particle
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Klaus Kirch 15 Tokyo, Feb 18, 2016
Only known LFV so far:
neutrino mixing
cLFV suppressed by
(dmn/mW)4 and thus
smaller than 10-50 SM not observable
accidentally small !?
Plenty of room for
new physics
Charged Lepton Flavor Violation
is small in the Standard Model
g
W-
m- nm ne
e-
Expect from SM:
BR(m-eg) < 10-50
Experimentally so far:
< 5.7 x 10-13
PRL110(2013)201801
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Klaus Kirch 16 Tokyo, Feb 18, 2016
cLFV Searches: Current Situation
The present best
limits on LFV
are from muon
experiments at PSI
m+ → e+ee
BR < 1 10-12
SINDRUM 1988
m- + Au → e- + Au
BR < 7 10-13
SINDRUM II 2006
m+ → e+ + g
BR < 5.7 10-13
MEG 2013
[90 % C.L.] SINDRUM
SINDRUM II MEG
10-14
10-10
10-4
Marciano, Mori, Roney
Most sensitive LFV search
MEGA@LANL
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Klaus Kirch 17 Tokyo, Feb 18, 2016
cLFV Searches: Current Situation
The present best
limits on LFV
come from PSI
muon experiments
m+ → e+ee
BR < 1 10-12
SINDRUM 1988
m- + Au → e- + Au
BR < 7 10-13
SINDRUM II 2006
m+ → e+ + g
BR < 5.7 10-13
MEG 2013
[90 % C.L.] SINDRUM
SINDRUM II MEG
10-14
10-10
10-4
Marciano, Mori, Roney
Next steps at PSI: MEG-II 4 x 10-14
Mu3e 10-15 (pE5) 10-16 (HiMB)
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Klaus Kirch 18 Tokyo, Feb 18, 2016
Improved analysis
applied to all data
MEG analysis Issues and Improvements in the m → e g analysis
• Alignment of Muon Stopping Target
• Alignment of LXe Detector
• Analysis of Annihilation-of-Flight (AIF)
Gamma Rays
• Recovery of Missing First Turns
Half data published
Expect publication soon:
2.4 x 10-12
5.7 x 10-13
2.8 x 10-11
sensitivity [2009-11] ~ 8 x 10-13
sensitivity [2009-13] ~ 5 x 10-13
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MEGII Status
7 x 107
muons/s
x2 resolution
everywhere
Key elements:
• Higher beam intensity
• Higher detector efficiency and
resolution
• Improved calibration methods
• New DAQ system
Design Construction PreEng Run Eng. Run Run
2013 2014 2015 2016 2017-20
Sensitivity [2017-20] ~ 4 x 10-14
MEG MEGII
u (mm)
v (mm)
w (mm)
ΔE/E (w< 2cm)
t (ps)
p (keV)
θ (mrad)
φ (mrad)
ε (%)
t (ps)
ε (%)
5
5
6
2.4
2.2
3.1
ΔE/E (w> 2cm)
2.4%
1.7%
1.1%
1.0%
67 <50
306 130
9.4
8.7
5.3
4.8
70 35
40 88
65 >70
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Klaus Kirch 20 Tokyo, Feb 18, 2016
MEGII Status
Single volume He:iC4H10
Better uniformity w/
12x12 VUV SiPM
7 x 107
muons/s
x2 resolution
everywhere
35 ps resolution
w/ multiple hits
Key elements:
• Higher beam intensity
• Higher detector efficiency and
resolution
• Improved calibration methods
• New DAQ system
Design Construction PreEng Run Eng. Run Run
2013 2014 2015 2016 2017-20
Sensitivity [2017-20] ~ 4 x 10-14
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Mu3e Status Key elements:
• Staged approach (here only
phase I up to 108 muons/s)
• Impressive momentum
resolutions
• Good timing also with minimal
amount of material
2013-5 2015-7 2017 2018-20
Sensitivity phase I [2018-20] ~ 10-15
Design Construction Eng Run Run Eng Run
(Final Sensitivity phase II [202x] ~ 10-16 )
Mupix det ect or
Fibre hodoscope
70 ps resolution
w/ single hit
~ 500 ps resolution
w/ double hits
thickness: < 0.3% X0
Tracking, integrate sensor and
readout in the same device: 50
um thick
1 layer: ~ 0.1% X0
Superconduct ing
solenoid Magnet
Homogeneous field
1T
Tile det ect or
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Klaus Kirch 22 Tokyo, Feb 18, 2016
HiMB Status
HIMB@SINQ HIMB@EH
Feasibility studies ongoing
• HIMB@SINQ: 3x1010 muon/s at 1.7 mA(SINQ) prior to capture.
Impractical as it would require removing beam-pipe constraints.
• HIMB@EH: a new solenoidal beamline coupled with a new 20 mm
slanted graphite target. Very promising:
O(1010 muon/s) seems feasible
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Klaus Kirch 23 Tokyo, Feb 18, 2016
MEG and Mu3e complementarity
See:
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Klaus Kirch 24 Tokyo, Feb 18, 2016
Search for new physics
Search for meg
g
m- e-
0~
m~
e~
High Energy High Intensity
direct production of new particle
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Klaus Kirch 25 Tokyo, Feb 18, 2016
Search for new physics
Search for nEDM
High Energy High Intensity
direct production of new particle
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Klaus Kirch 26 Tokyo, Feb 18, 2016
Search for new physics
Search for nEDM
High Energy High Intensity
direct production of new particle
Mass reach: few TeV Mass reach: 1 - 1000 TeV
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Klaus Kirch 27 Tokyo, Feb 18, 2016
Electric Dipole Moments are small in
the Standard Model
Leptons: 4th order electro-weak
F. Hoogeveen: The Standard Model Prediction for the Electric Dipole Moment of the Electron, Nucl. Phys. B 241 (1990) 322
T
Expect from SM,
approximately:
de ≤ 10-38 e•cm
dm ≤ 10-36 e•cm
dt ≤ 10-35 e•cm
Experimentally so far:
de< 9 x 10-29 e•cm
dm< 2 x 10-19 e•cm
dt< 3 x 10-17 e•cm
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Klaus Kirch 28 Tokyo, Feb 18, 2016
Neutron, Proton, ..
T
Expect from SM:
dn < 10-30 e•cm
Experimentally so far:
< 2.9 x 10-26 e•cm
Electric Dipole Moments are small in
the Standard Model
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Klaus Kirch 29 Tokyo, Feb 18, 2016
10-26
10-20 10-20
10-26
1950 2000
ED
M u
pper
limit [e
cm
]
[e cm] Caveat:
The strong CP problem
.
dn ≈ 10-16 e cm • qQCD
qQCD < 10-10
~
LQCD ≈ LQCD + g2/(32p2) qQCDGG ~
Why is qQCD so small ?
QC
D
RAL-Sussex-ILL
dn < 2.9 x 10–26 ecm C.A.Baker et al.,
PRL 97 (2006) 131801
Smith, Purcell, Ramsey
PR108(1957)120
qQCD=0
accidentally small !?
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Klaus Kirch 30 Tokyo, Feb 18, 2016
The SUSY CP problem
.
10-26
10-20 10-20
10-26
1950 2000
ED
M u
pper
limit [e
cm
]
[e cm]
dn ≈ 10-23 e cm ( )sinfSUSY
300 GeV/c
MSUSY
2 2
SU
SY
Why is fSUSY so small ?
See: Pospelov, Ritz,
Ann. Phys. 318(2005)119
for MSUSY = 500GeV, tan b = 3
(for neutron and electron!)
(this is testing M already to 10TeV and you
may also ask: why are the masses so huge?)
pre LHC
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Klaus Kirch 31 Tokyo, Feb 18, 2016
The SUSY CP problem
.
10-26
10-20 10-20
10-26
1950 2000
ED
M u
pper
limit [e
cm
]
[e cm]
dn ≈ 10-23 e cm ( )sinfSUSY
300 GeV/c
MSUSY
2 2
SU
SY
Why is fSUSY so small ?
(for neutron and electron!)
(this is testing M already to 10TeV and you
may also ask: why are the masses so huge?)
A. Ritz,
update 2013
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Klaus Kirch 32 Tokyo, Feb 18, 2016
The SUSY CP problem
.
10-26
10-20 10-20
10-26
1950 2000
ED
M u
pper
limit [e
cm
]
[e cm]
dn ≈ 10-23 e cm ( )sinfSUSY
300 GeV/c
MSUSY
2 2
SU
SY
Why is fSUSY so small ?
Pospelov, Ritz, Ann. Phys. 318(2005)119
for MSUSY = 500GeV, tan b = 3
(for neutron and electron!)
(this is testing M already to 10TeV and you
may also ask: why are the masses so huge?)
A. Ritz,
update 2014
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Klaus Kirch 33 Tokyo, Feb 18, 2016
The SUSY CP problem
.
10-26
10-20 10-20
10-26
1950 2000
ED
M u
pper
limit [e
cm
]
[e cm]
dn ≈ 10-23 e cm ( )sinfSUSY
300 GeV/c
MSUSY
2 2
SU
SY
Why is fSUSY so small ?
Pospelov, Ritz, Ann. Phys. 318(2005)119
for MSUSY = 500GeV, tan b = 3
(for neutron and electron!)
(this is testing M already to 10TeV and you
may also ask: why are the masses so huge?)
A. Ritz,
update 2016
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Klaus Kirch 34 Tokyo, Feb 18, 2016
The BAU CP Problem
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Klaus Kirch 35 Tokyo, Feb 18, 2016
Nature has probably violated CP when
generating the Baryon asymmetry !?
Sakharov 1967:
B-violation
C & CP-violation
non-equilibrium
[JETP Lett. 5 (1967) 24]
* WMAP + COBE, 2003
nB / ng = (6.1 ± ) x 10-10 0.3 0.2
Observed*:
(nB-nB) / ng = 6 x 10-10
SM expectation:
(nB-nB) / ng ~ 10-18
_
_
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Klaus Kirch 36 Tokyo, Feb 18, 2016
UCN sources [some belong to specific experiments]
Operating:
ILL PF-2 (turbine)
LANL (sD2)
PSI (sD2)
TRIGA Mainz (sD2)
RCNP (SF-He)
ILL SUN2 (SF-He)
ILL: Sun1 GRANIT
[NIST: lifetime]
R&D and construction
ILL SuperSUN
TRIUMF/RCNP
PNPI WWR-M
NCSU PULSTAR
FRM-2
SNS-EDM
Possible projects
J-PARC
PIK
ESS
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Klaus Kirch 37 Tokyo, Feb 18, 2016
Neutron EDM projects
Operating:
PNPI, ILL@ILL (result 2013/14, upgrading)
nEDM@PSI (2018 upgrade to n2EDM)
R&D and construction
@RCNP/TRIUMF
@FRM-2
@SNS
@PNPI
@LANL
Possible future projects
@J-PARC
@PIK
@ESS
Ne
w
ph
ys
ics
(Essentially all of them aiming at 1-2 orders of magnitude improvement)
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Klaus Kirch 38 Tokyo, Feb 18, 2016
All nEDM competitive today
use ultracold neutrons – UCN
move with velocities of few m/s
have kinetic energies of order 100 neV
strong magnetic gravitation
60 neV T-1 300 neV
Fermi potential VF Vm = -mB Vg = mngh
100 neV m-1
5 T field -> 300 neV 3 m up -> 300 neV
V
En < 300 neV
UCN: similar to ideal gas with temperatures of milli-Kelvin (very dilute and not in thermal equilibrium with walls)
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Klaus Kirch 39 Tokyo, Feb 18, 2016
How to measure the neutron
(or other) electric dipole moment ?
B E
hn = 2 (μB+dnE)
hn = 2 (μB- dnE)
hDn = 4 dn E
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Klaus Kirch 40 Tokyo, Feb 18, 2016
Ramsey’s method with UCN
frf
frf
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Klaus Kirch 41 Tokyo, Feb 18, 2016
UCN-Source - 1st test: 12/2010 - Safety approval: 06/2011 - UCN start 08/2011 - Reliable performance 2012 - UCN to nEDM since 2012 -> intensity 90x over 2010 - Increased duty factor 2015: 20 40 mA average - 2016: towards 60mA
nEDM
590 MeV Proton Cyclotron 2.2 .. 2.4 mA Beam Current
Excellent performance of HIPA and regular beam delivery to UCN
Ultracold Neutron Source & Facility
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Klaus Kirch 42 Tokyo, Feb 18, 2016
The PSI UCN source
pulsed 1.3 MW p-beam 600 MeV, 2.2 mA, 1% duty cycle
spallation target (Pb/Zr) (~ 8 neutrons/proton)
heavy water moderator → thermal neutrons 3.6m3 D2O cold UCN-converter
~30 dm3 solid D2 at 5 K
tank
7 m
DLC coated UCN storage vessel height 2.5 m, ~ 2 m3
UCN guides towards experimental areas 8.6m(S) / 6.9m(W)
SV-shutter
cryo-pump
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Klaus Kirch 43 Tokyo, Feb 18, 2016
The PSI UCN source
22.07.2010
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Klaus Kirch 44 Tokyo, Feb 18, 2016
Getting routine with operation
40 mA average beam current
can result in max. 1 mAh / day
nEDM operates with approx.
250 pulses per day
1 typical pulse ~ few seconds, 5E16 p on target, 4E17 spallation n, 1E9 UCN
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Klaus Kirch 45 Tokyo, Feb 18, 2016
Continuous improvement under way:
UCN per proton pulse 2s Normkicks
Standard operating Pulse
Norm Pulse
UC
N C
ou
nts
/s
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Klaus Kirch 46 Tokyo, Feb 18, 2016
Continuous improvement under way
2s Normkicks
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Klaus Kirch 47 Tokyo, Feb 18, 2016
UCN source – nEDM counts UCN counts in nEDM experiment during 2015
UCN counts after
180s of storage
in the nEDM
precession chamber
Main features:
- operation / failsafe
- fast UCN output
decrease
- Recovery after
conditioning
- Overall positive
trend
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Klaus Kirch 48 Tokyo, Feb 18, 2016
Installing nEDM
at PSI in 2009
Coming from ILL
Sussex-RAL-ILL collaboration
PRL 97 (2006) 131801
nedm.web.psi.ch
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Klaus Kirch 49 Tokyo, Feb 18, 2016
The nEDM spectrometer
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Klaus Kirch 50 Tokyo, Feb 18, 2016
The nEDM spectrometer
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Klaus Kirch 51 Tokyo, Feb 18, 2016
Features of nEDM@PSI Hg-199 co-magnetometer
improved S/N by factor >4
laser read-out proven, being implemented
CsM array
16 scalar sensors in operation (6 HV)
vector CsM proven
B-field
homogeneity (T2~1000s)
reproducibility (~50pT), after degaussing
(~200pT)
Simultaneous spin analysis
Known systematics well under control
down to ~2 x 10-27 ecm
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Klaus Kirch 52 Tokyo, Feb 18, 2016
Frequency ratio R
UCN 199Hg
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Klaus Kirch 53 Tokyo, Feb 18, 2016
Magnetic moments
γn
γHg
S. Afach et al., PLB 739 (2014) 128
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Klaus Kirch 54 Tokyo, Feb 18, 2016
Spin-dependent exotic interactions
PhD thesis
B. Franke, 2014 S. Afach et al., PLB 745 (2015) 58
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Klaus Kirch 55 Tokyo, Feb 18, 2016
Spin-echo spectroscopy A spin-echo recovers energy
dependent dephasing for
T = 2t1 in a magnetic field
with vertical gradient.
gz
S. Afach et al., PRL114(2015)162502
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Klaus Kirch 56 Tokyo, Feb 18, 2016
Towards new limits Neutron EDM search N
2dσ
αET N
Once nEDM runs out of steam statistically,
it will be replaced by n2EDM (~2018)
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Klaus Kirch 57 Tokyo, Feb 18, 2016
1.7×10-26 ecm
Towards new limits Neutron EDM search
The slope determines
the path forward
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Klaus Kirch 58 Tokyo, Feb 18, 2016
• Expect new MEG result shortly
• UCN source performance continuously improving
• New nEDM result 2016/17
• Lambshift 2S-2P in mHe being analyzed
• HiMB feasibility study under way
• MEG II and Mu3e progress very promising
• Phase space compression experiment muCool
demonstrated milestones …
see you perhaps at PSI2016?
Exciting times ahead
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Klaus Kirch 59 Tokyo, Feb 18, 2016
www.psi.ch/particle-zuoz-school www.psi.ch/psi2016
LTP organizes the PSI20xy conferences
and the Particle Physics Zuoz school
August 14 – 20, 2016 October 17 – 20, 2016
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Klaus Kirch 60 Tokyo, Feb 18, 2016 Picture: K. Schuhmann
Thank you!