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Progress on the final TWIST measurement of James Bueno, University of British Columbia and TRIUMF
P
on behalf of theTriumf Weak Interaction Symmetry Test
Outline
• Muon production and decay
• Previous measurements of
• Sources of depolarisation,
and their simulation.– Depolarisation in fringe field of solenoid.– Depolarisation in the muon stopping target.
P
James Bueno, WNPPC 2008, 15 February
1/20
Muon production and
James Bueno, WNPPC 2008, 15 February
P
hh
Muons from stationary
pion decay are perfectly
polarised
(for massless neutrinos)
TWIST only accepts a narrowmomentum range
muon beam is highly polarised
2/20
Muon decay and
James Bueno, WNPPC 2008, 15 February
P
e
e
cosP,xF,,xF
cosddx
dASIS
2
TWIST measures
e+ energy (x) and
angle (θ) relative
to muon spin.
3/20
Muon decay and
James Bueno, WNPPC 2008, 15 February
P
e
e
cosP,xF,,xF
cosddx
dASIS
2
TWIST measures
e+ energy (x) and
angle (θ) relative
to muon spin.
determines forward-
backward asymmetry
3/20
Muon decay and
James Bueno, WNPPC 2008, 15 February
P
e
e
cosP,xF,,xF
cosddx
dASIS
2
TWIST measures
e+ energy (x) and
angle (θ) relative
to muon spin.
determines forward-
backward asymmetry appears as an
inseparable productP
3/20
Physics motivation
muon handedness
9
16
3
11
2
1QR
SM predicts LH muon decays to LH positron.
Probability of RH muon decay to a LH
or RH positron is
James Bueno, WNPPC 2008, 15 February
4/20
Physics motivation
muon handedness left-right symmetric models
9
16
3
11
2
1QR
SM predicts LH muon decays to LH positron.
Probability of RH muon decay to a LH
or RH positron is
cosWsinWW
sinWcosWW
21R
21L
4
2
1
2
2
12
m
m
m
m4P1
James Bueno, WNPPC 2008, 15 February
4/20
Previous measurements of
1987, Beltrami et al. (PSI)1.0027 ± 0.0079 (stat.)
± 0.0030 (syst.)
2006, Jamieson et al. (TWIST, TRIUMF)
1.0003 ± 0.0006 (stat.)
± 0.0038 (syst.)
P
James Bueno, WNPPC 2008, 15 February
Standard model, 1,1P
5/20
Previous measurements of
1987, Beltrami et al. (PSI)1.0027 ± 0.0079 (stat.)
± 0.0030 (syst.)
2006, Jamieson et al. (TWIST, TRIUMF)
1.0003 ± 0.0006 (stat.)
± 0.0038 (syst.)
2004, Jodidio et al. with TWIST ρ, δ (Indirect)
0.9960 < < 1.0040
(90% confidence)
P
James Bueno, WNPPC 2008, 15 February
Standard model, 1,1P
P
5/20
Previous measurements of
1987, Beltrami et al. (PSI)1.0027 ± 0.0079 (stat.)
± 0.0030 (syst.)
2006, Jamieson et al. (TWIST, TRIUMF)
1.0003 ± 0.0006 (stat.)
± 0.0038 (syst.)
2004, Jodidio et al. with TWIST ρ, δ (Indirect)
0.9960 < < 1.0040
(90% confidence)
2009, final result
from TWIST (goal)± 0.0003 (stat.)± 0.0010 (syst.)
P
James Bueno, WNPPC 2008, 15 February
Standard model, 1,1P
P
5/20
Previous measurements of
1987, Beltrami et al. (PSI)1.0027 ± 0.0079 (stat.)
± 0.0030 (syst.)
2006, Jamieson et al. (TWIST, TRIUMF)
1.0003 ± 0.0006 (stat.)
± 0.0038 (syst.)
2004, Jodidio et al. with TWIST ρ, δ (Indirect)
0.9960 < < 1.0040
(90% confidence)
2009, final result
from TWIST (goal)± 0.0003 (stat.)± 0.0010 (syst.)
P
James Bueno, WNPPC 2008, 15 February
Standard model, 1,1P
P Previous TWIST direct measurement
limited by uncertainties in simulating P
5/20
TWIST measurement of P
1
x
= E/Emax
-1
+10cos θ
Michel spectrum
from real data
Spectrum from
GEANT simulationhidden
difference in is measuredP
Spectra from decay (depolarised) μ are compared depolarisation in simulation must match data
P
0
6/20
Sources of depolarisation
James Bueno, WNPPC 2008, 15 February
symmetric tracking volume
solenoid fringe field
depends on trajectoryP
7/20
Sources of depolarisation
James Bueno, WNPPC 2008, 15 February
high purity metal
target to stop muons
symmetric tracking volume
depends on timeP
solenoid fringe field
depends on trajectoryP
7/20
Simulating the depolarisation
James Bueno, WNPPC 2008, 15 February
Beam is measuredby time expansion
chambers BEFOREthe fringe field
symmetric tracking volume
7/20
XY
Simulating the depolarisation
James Bueno, WNPPC 2008, 15 February
Beam is measuredby time expansion
chambers BEFOREthe fringe field
Time dependence ofe+ forward-backward
asymmetry gives in target tP
symmetric tracking volume
7/20
XY
Simulating muon trajectories
James Bueno, WNPPC 2008, 15 February
1. Measure each muon’s
position and angle with
time expansion chambers.
projection
in x
8/20
Simulating muon trajectories
James Bueno, WNPPC 2008, 15 February
1. Measure each muon’s
position and angle with
time expansion chambers.
projection
in x
2. Correct angles for
multiple scattering.
3. Simulate muons with
GEANT and track spin to
predict at target.P
Uncertainties due to beam instability, initial position& angle of beam, position & shape of B-field.
8/20
Beam stability (1 of 2)
James Bueno, WNPPC 2008, 15 February
During data acquisition, we needed a
stable muon beam for weeks on end.
9/20
Beam stability (1 of 2)
James Bueno, WNPPC 2008, 15 February
During data acquisition, we needed a
stable muon beam for weeks on end.
And a method of detecting beam
instabilities without the time expansion
chambers in place.
(too much multiple scattering)
9/20
Beam stability (2 of 2)
James Bueno, WNPPC 2008, 15 February
For 2006/7, internal beamspots are fit to a helix.
Helix fit parameters
indicate position and
momentum.
most of
data set
beam
instability
10/20
5mm
Misalignment uncertainties
James Bueno, WNPPC 2008, 15 February
For 2006/2007 data, the beam was steered
onto the solenoid axis.
2004 beam
2006/7 beam
y (cm)
11/20
Misalignment uncertainties
James Bueno, WNPPC 2008, 15 February
For 2006/2007 data, the beam was steered
onto the solenoid axis.
2004 beam
2006/7 beam
y (cm)
2006
2004
Sensitivity to misalignmentsis now reduced
11/20
Spin tracking in the B-field
James Bueno, WNPPC 2008, 15 February
To validate GEANT’s spin tracking: two weeks
of low data taken in 2006/7.
nominalsteered
at angle
P
12/20
Spin tracking in the B-field
James Bueno, WNPPC 2008, 15 February
To validate GEANT’s spin tracking: two weeks
of low data taken in 2006/7.
nominalsteered
at angle
inside detector
nominal
steered
P
12/20
Spin tracking in the B-field
James Bueno, WNPPC 2008, 15 February
To validate GEANT’s spin tracking: two weeks
of low data taken in 2006/7.
nominalsteered
at angle
inside detector
nominal
steered
P
Validation (in progress now) will require:
SIMULATION
steerednominal
DATA
steerednominal PPPP
12/20
Stopping target depolarisation
James Bueno, WNPPC 2008, 15 February
Ideally, the muons would not depolarise at the
stopping target
(it’s 99.999% pure aluminium, or silver).
However, an individual muon spin can interact
with local magnetic fields and reverse sign.
13/20
Stopping target depolarisation
James Bueno, WNPPC 2008, 15 February
The simulation must include the correct model
for in the target. tP
14/20
Stopping target depolarisation
James Bueno, WNPPC 2008, 15 February
The simulation must include the correct model
for in the target. tP
TWIST result for silver
theoretically
preferred
atexp0PtP
also possible
2btexp0PtP
14/20
Stopping target depolarisation
James Bueno, WNPPC 2008, 15 February
The simulation must include the correct model
for in the target. tP
TWIST result for silver
theoretically
preferred
atexp0PtP
also possible
2btexp0PtP no data below
~ 1 μs (or above 10 μs)
A subsidiary experiment would be helpful…
14/20
Subsidiary muSR experiment
collimatorbackward
e+ counter
target
forward e+
counter
trigger scintillatorsSchematic, not to scale
15/20
Subsidiary muSR experiment
collimatorbackward
e+ counter
target
forward e+
counter
trigger scintillatorsSchematic, not to scale
e
15/20
Subsidiary muSR experiment
Advantages:• Higher rate (~30kHz compared to ~3kHz)• Larger time fiducial
(~5 ns 14 μs, compared to ~1 μs ~9 μs).
16/20
James Bueno, WNPPC 2008, 15 February
Subsidiary muSR experiment
Advantages:• Higher rate (~30kHz compared to ~3kHz)• Larger time fiducial
(~5 ns 14 μs, compared to ~1 μs ~9 μs).
Disadvantages:• Background from beam positrons.• A fraction of muons stop in the scintillator.
16/20
James Bueno, WNPPC 2008, 15 February
Subsidiary muSR experiment
Unfortunately, still no discrimination betweenand atexp0PtP 2btexp0PtP
17/20
Subsidiary muSR experiment
exp(-at)Aluminium
a (x10-6ns-1)
Silver
a (x10-6ns-1)
TWIST 1.4 ± 0.1 1.1 ± 0.3
muSR 1.7 ± 0.2 1.2 ± 0.2
Unfortunately, still no discrimination betweenand atexp0PtP 2btexp0PtP
17/20
Subsidiary muSR experiment
exp(-at)Aluminium
a (x10-6ns-1)
Silver
a (x10-6ns-1)
TWIST 1.4 ± 0.1 1.1 ± 0.3
muSR 1.7 ± 0.2 1.2 ± 0.2
Unfortunately, still no discrimination betweenand
Experiment confirmed no fast depolarisationbetween ~5 ns and 1 μs, and results are
consistent with TWIST.
atexp0PtP 2btexp0PtP
17/20
Using target PCs in TWIST
proportional chambers
closest to stopping target
stopping
target
μ can stop
in chamber gas
18/20
PC6PC5
Using target PCs in TWIST
proportional chambers
closest to stopping target
stopping
target
μ can stop
in chamber gas
pulse width in final PCgreater for muons that
stop here (moreenergy deposited)
18/20
PC6PC5
Using target PCs in TWIST
proportional chambers
closest to stopping target
stopping
target
μ can stop
in chamber gas
pulse width in final PCgreater for muons that
stop here (moreenergy deposited)
PC 5 (ns) PC 6 (ns)
18/20
PC6PC5
Using target PCs in TWIST
proportional chambers
closest to stopping target
stopping
target
μ can stop
in chamber gas
pulse width in final PCgreater for muons that
stop here (moreenergy deposited)
deep cut selectstarget stop μ
PC 5 (ns) PC 6 (ns)
18/20
PC6PC5and rejects
these
Summary
James Bueno, WNPPC 2008, 15 February
• The final measurement is dominated by uncertainties in simulating .
• Validation of the spin tracking is well underway.• Improvements in data acquisition in 2006/7 will
reduce uncertainties.
19/20
PP
P
Summary
James Bueno, WNPPC 2008, 15 February
• The final measurement is dominated by uncertainties in simulating .
• Validation of the spin tracking is well underway.• Improvements in data acquisition in 2006/7 will
reduce uncertainties.• Subsidiary muSR experiment has confirmed
no fast depolarisation exists
(this could not be measured by TWIST).• Time dependent depolarisation uncertainties can
be minimised by selecting genuine target stops.
19/20
PP
P
James Bueno, WNPPC 2008, 15 February
Alberta
Ryan Bayes*† Glen Marshall Andrei Gaponenko**
Yuri Davydov Dick Mischke Peter Kitching
Wayne Faszer Mina Nozar Robert MacDonald*
Makoto Fujiwara Konstantin Olchanski Maher Quraan
David Gill Art Olin†
Alexander Grossheim Robert Openshaw British Columbia
Peter Gumplinger Jean-Michel Poutissou James Bueno*
Anthony Hillairet*† Renée Poutissou Mike Hasinoff
Robert Henderson Grant Sheffer Blair Jamieson**
Jingliang Hu Bill Shin‡‡
Texas A&M
Regina Montréal Carl Gagliardi
Ted Mathie Pierre Depommier Jim Musser**
Roman Tacik Bob Tribble
Valparaiso
Kurchatov Institute Don Koetke
Vladimir Selivanov Shirvel Stanislaus
TRIUMF
* graduate student, ** graduated
† also UVic, ‡‡ also Saskatchewan
TWIST is supported in part by
the Natural Sciences and
Engineering Research Council
and the National Research
Council of Canada, the Russian
Ministry of Science, and the
U.S. Department of Energy.
Computing resources for the
analysis are provided
by Westgrid.
The TWIST collaboration 20/20