Polarization for precision measurements
Torsten Soldner
Institut Laue Langevin
Polarization – Definition
More precisely: spin polarization
• Degree to which the spin of particles is aligned with a given direction
• For spin ½ particles:
• Property of an ensemble of particles, not of a single particle!
• Polarization vector:
NN
NNP
NP
N
i i
1
Asymmetry measurements
epPAW
1d
d
d
BeamDetector
d 1 epPAN
BeamDetectorBeam
BeamDetector
d )(d )( ee prPprP
BeamDetector
d 1 epPAN
BeamDetector
d
epPA
NN
NN
Solution I – Detector averages beam
Beam
averageDetector average
Detector average of P
Beam average of P
Beam
averageDetector average
Solution II – Polarization homogeneos
Beam
averageDetector average
Detector average of P
Beam average of P
Beam
averageDetector average
Content
• Techniques for polarization and spin flipping
• Polarization analysis
• Pushing P
Polarization – Supermirrors
B
10-7eV
U
10-7eV10-7eV
BUU
opt
Match index of refraction
Increase critical angle(see optics lecture)
Example: m=4 FeSi super mirror
Picture from Swiss Neutronics web page
Matching works better for CoTi, but activation worse
Note expanded scale for P
SM bender – Dependencies
00 qq
Wavelengthdependence
Angledependence
SM bender – angular dependence
-8 -6 -4 -2 0 2 4 6 8 100.93
0.94
0.95
0.96
0.97
0.98
0.99
1.00
AP
Position [mrad]
Single Analyzer
Crossed Analyzer
Old example, modern polarizers are much better
SM bender – wavelength dependence
Old example, modern polarizers are much better
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 150.75
0.80
0.85
0.90
0.95
1.00
1.05
AP
[A]
Single Analyzer
Crossed Analyzer
3He spin filter
Angle-independent (cos(θ))Pn up to 100%
PHe, Pn drop in time dependent
σc,0 = 5333(7) barn
σc↑↓/ σc,0 =1.010(32)(often assumed that σc↑↑ = 0 but known only on % level)
σc↑↓>>σc↑↑
n+3He t + p
)1(]He[exp2
1He0 PlT
He)(tanh POPn lpOÅ cmbar
0733.0)( opacity
He
)(
n )(coshe POT O
0e)0()( HeHe
T
t
PtP
relaxation of hyperpolarized 3He
3He spin filter
PHe=0.7, p=2bar, l=10cm
He)(tanh POPn
3He spin filter
PHe=0.7, p=2bar, l=10cm
He
)(
n )(coshe POT O
Cells
Techniques
MEOP (metastability exchange optical pumping)
• Pump 3He to metastable state
• Polarize nuclei
• Works at mbar pressure offline pumping, compression
SEOP (spin exchange optical pumping)
• Pump electrons in alkali metal
• Transfer to 3He by collision
• Works at bar pressure online pumping
• Strong performance loss in high neutron flux
Flipper I – Current sheet
Non-adiabatic transition
B
B
• Good for fast neutrons, bad for slow (adiabaticity)• Difficult to adjust:
OFF: adiabatic transport ON: non-adiabatic transition, no other field components
• Requires material in the beam, scattering may be current-dependent
Typical parameters:Wire: D = 1mmCurrent: I = 10 A
Flippers II – Adiabatic fast passage
1 2 3 4 5 6 7 8 9 10 11 12 13 14 150.985
0.990
0.995
1.000
1.005
Radio Frequency Flipper
<f> = 0.9993±0.0001
Current Sheet Fliper
Flip
pe
r e
ffic
ien
cy
[A]
ω
Frame rotating with ω:
ω=γBR
ΔB=B(x)-BR
B1
B0(x)
xB1
Typical values: f=ω/2π=50 kHz, BR=17 G
Flippers III – Small-band
Mezei flipper:Non-adiabatic transition, adiabatic rotation
• For π/2 flip (as needed for EDM or spin echo experiments)• Works only for fixed wavelength (tunable to λ at pulsed beam)
More complex configuration for arbitrary rotation angle
Resonance spin flipperSee Florian’s lecture
Polarization Analysis
A handy formalism I
Particles spin up
Particles spin down
1
1
2
nBUnpolarized beam
P
P
10
01PPolarizer
P
Pn
1
1
2PB P
NN
NN
A handy formalism II
Particles spin up
Particles spin down
1
1
2
nBUnpolarized beam
P
P
10
01PPolarizer
FF
FF
1
1FSpin flipper
)21(1
)21(1
2 FP
FPnFPB )21( FP
NN
NN
F Spin flip efficiency ε = 1-F Spin flip inefficiencyf = 2F-1 Flipper efficiency (modification of beam polarization
by flipper)
A handy formalism III
Particles spin up
Particles spin down
1
1
2
nBUnpolarized beam
P
P
10
01PPolarizer
FF
FF
1
1FSpin flipper
ddDDetector Insensitive to polarization
A
A
10
01AAnalyzer
Detection efficiencyndN (...)... BD
Detected neutrons:
Polarization analysis I – One flipper
B P F A D
Flipper off dbAPN )1(0 DAPB
Flipper on dbAPFAPN )21(1 DAFPB
)1(110
10
FAP
APF
NN
NN
)21(1
1
1
0
FAP
AP
N
Nr
APF cannot be separated
Flipping ratio10
10
1
1
NN
NN
r
r
Polarization analysis II – Two flippers
B P F1 A DF2
PBFFAD
PBFAD
PBFAD
PBAD
1
1
211
201
10
00
N
N
N
N
0001
10111 1
2
1
NN
NNF
0010
01112 1
2
1
NN
NNF
01101100
01001000
NNNN
NNNNAP
AP cannot be separatedF1 and F2 can
Requires a lot of statistics
White
Black
Black
White
Polarization analysis with SM?
F1 F2P1 P2
0001
10111 1
2
1
NN
NNF
0010
01112 1
2
1
NN
NNF
01101100
01001000
NNNN
NNNNAP
APP ________ (assuming A=P) does not work, strictly speaking
)()()()( 2121 PPPP
P is property ofdevice AND beam
Polarization analysis III – Analyzer flip
B P F A D
AP cannot be separatedF can
10
20
NN
NNF
10
10
NN
NNAP
PBFAD
PBAD
PBAD
)(
)(
)(
2
1
0
AN
AN
AN
White
Black
Black
Works for 3He analyzerWe have 3He flippers with ε ~ 3∙10-6
This can be measured easily by performing many flips
He)(tanh POPn
Example X-SM geometry
0 2 4 6 8 10 12 14 16 18 20-0,950
-0,955
-0,960
-0,965
-0,970
-0,975
-0,980
-0,985
-0,990
-0,995
-1,000
Pola
riza
tio
n
Neutron wavelength (A)
<P> = (99.72 +/- 0.10)%
p0 5.5 Bar
p1 4.0 Bar
p2 2.1 Bar
p3 1.5 Bar
p4 1.0 Bar
p5 0.67 Bar
Spectrum
Used in PERKEO II, Mund et al, PRL 110 (2013) 172502
Analysis of inhomogeneous polarization
Accurate scan of beam:• Same areas for intensity
and polarization scansAccurate average
Exploit features of 3He:• No angular dependence• large area average
possible
Pushing P
Combining polarizers?
Polarisers not independent
)(),()(
)(),()(
22
2
11
1
RRfP
RRfP
)()()()( 2121 PPPP
The X-SM geometryalso known as “crossed”, but different meaning in optics
Polarizers independent
)(),()(
)(),()(
22
2
11
1
yyy
xxx
RRfP
RRfP
yxyxyxyx PPPP
)()()()( 21,21
Polarization analysis with X-SM?
F1 F2P1 P2
0001
10111 1
2
1
NN
NNF
0010
01112 1
2
1
NN
NNF
01101100
01001000
NNNN
NNNNAP
yxyxyxyx PPPP
)()()()( 21,21
A and P independent, but numbers depend on beam (incoming divergence…) Cannot separate
P is property ofdevice AND beam
But very powerful polarizer
n
P1 P2R
BB
BY
ZX
n
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 150.75
0.80
0.85
0.90
0.95
1.00
1.05
P
[A]
Measured single Polarizer
Prediction for Crossed Geometry
2112 TTT
Predictable Polarisation...
...and Transmission
21
2112
1 PP
PPP
)1)(1(2
11 2112 PPP
adiabatic rotation
Measured performance
-8 -6 -4 -2 0 2 4 6 8 100.93
0.94
0.95
0.96
0.97
0.98
0.99
1.00
AP
Position [mrad]
Single Analyzer
Crossed Analyzer
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 150.75
0.80
0.85
0.90
0.95
1.00
1.05
AP
[A]
Single Analyzer
Crossed Analyzer
(with old polarizers)
)1)(1(2
11 2112 PPP
Pi = 0.95 expect P12 =0.999
Much more than measured!
But:
1 2 3 4 5 6 7 8 9 10 11 12 13 14 150.96
0.97
0.98
0.99
1.00
AP
[A]
Fields in Polarizer / Analyzer
BP=200 G, B
A=200 G
BP=200 G, B
A=350 G
BP=350 G, B
A=350 G
State of the art ILL SM Polariser
Magnetic housing field 1 kG
Limit of X-SM polarizer
Magnetic layers still not completely saturated
X-SM polarizer with X-SM analyzer:
Accuracy of 3He spin filters
– The opaque test bench –
P>99.995% A>99.995%F>99.999%
He)(tanh POP He)(tanh POA
Idea:Clean systematics by pure ↑ beam
Motivation:• Test ultimate performance of 3He spin filters• Precision characterization of polarizing elements
Analysing Power of 3He
Befilter
Chopper
→ Accuracy better than 10-4
l = 14cmpHe = 1.69 bar(and: 1.0 bar, 1.4 bar)
He)(tanh POP
C. Klauser, PhD thesis (2013)
AFP Flipper
Befilter
Chopper
→ F > 99.99%from 3 to 9 Å
10
2011NN
NNf
C. Klauser, PhD thesis (2013)
2
1
0
N
N
N
Detects only unflippedneutrons very sensitive
Depolarisation in super mirrors
Befilter
Selector Electromagnet0.85T
(Basic reflectometer)
C. Klauser, PhD thesis (2013)
Depolarisation in super mirrors
(Basic reflectometer)
C. Klauser, PhD thesis (2013)
Depolarization can be reduced by • higher magnetizing
field• lower m• choice of material
SuperADAM
Reflectometer with polarization analysis
Origin of depolarisation in SMs
Off-specularscattering: scattering by domains that are not aligned
Can be reduced by increasing the magnetizing field
Apply to X-SM
Befilter
Selector Electromagnet0.85T
(Basic reflectometer)
C. Klauser, PhD thesis (2013)
0.9970
0.9975
0.9980
0.9985
0.9990
0.9995
1.0000
0 0.2 0.4 0.6 0.8 1
AP
Magnetising-Field 1st Mirror [Tesla]
2.0 FeSi
2.0 CoTi
→ P = 99.970(3)%achieved with SMs only
Summary
Super mirrors
• Constant in time
• Wavelength dependent
• Angle dependent
98% routine
99.7% with X-SM
99.97% with pushed X-SM
3He spin filters
• Changes in time
• Wavelength dependent
• Negligible angle dependence
> 99.99% possible
AFP flipper
> 99.99% possible in λ range
10-4 accuracy achievable but requires careful design of polarizer and analysis