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Spin Tracking Studies for Polarimetry at the ILC
Moritz Beckmann, Jenny List
DESY - FLC
visiting SLAC May-August 2010
LC-Forum
July 14, 2011
IntroductionPolarization
• Here: longitudinal polarization (alongbeam axis)
• P = pR − pL ∈ [−1,+1]
• Beam with 90% R (and thus 10% L)→ 80% polarization
Moritz Beckmann LC-Forum July 14, 2011 2/ 16
IntroductionPolarimetry at the ILC
• Polarization measurement with 0.25 % uncertainty
• Calibration to 0.1% using collision data
• Must understand spin diffusion/depolarization to 0.1%(further) spin tracking studies required
Moritz Beckmann LC-Forum July 14, 2011 3/ 16
Simulation
• This study: ILC
• Could be used for other projects (e.g. CLIC) as well, if fedwith corresponding beamline design / parameters
Moritz Beckmann LC-Forum July 14, 2011 4/ 16
Spin tracking
• Spin propagation in electromagnetic fields isdescribed by T-BMT equation
d
dt~s = ~Ω
(~E (~r , t), ~B(~r , t), ~p ,m , a
)×~s
• Approximation (~B⊥ only): precession
θspin = (aγ + 1) · θorbit
Electrons at 250 GeV: aγ + 1 ≈ 568 B
a ≡ g−22 : anomalous gyro-magnetic moment
γ = Em
Moritz Beckmann LC-Forum July 14, 2011 5/ 16
Beam Delivery System des ILC
Latest available beamline design (SB2009 Nov10 lattice)
Moritz Beckmann LC-Forum July 14, 2011 6/ 16
Idealized Lattice
• 10 000 simulated particles, spins parallel to z-axis
• Perfect magnet alignment, no collision effects
• In the following: look only at polarimeters und IP
distance from IP [m]-3000 -2500 -2000 -1500 -1000 -500 0
lon
g. p
ola
riza
tio
n
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
UP IP,DP
doglegcollimation energy
UP/DP: up-/downstream polarimeter
Moritz Beckmann LC-Forum July 14, 2011 7/ 16
Idealized Lattice
• 10 000 simulated particles, spins parallel to z-axis
• Perfect magnet alignment, no collision effects
• No significant depolarization at the points of interest
distance from IP [m]-1680 -1660 -1640 -1620
lon
g. p
ola
riza
tio
n
0.6
0.7
0.8
UP
distance from IP [m]0 20 40 60 80 100 120 140
0.6
0.7
0.8
IP DP
UP/DP: up-/downstream polarimeter
Moritz Beckmann LC-Forum July 14, 2011 8/ 16
Misalignments
• Magnets between polarimeters misaligned⇒ particles see field 6= design field⇒ affects spin orientation
• Static and time-dependent misalignments
• Beam orbit correction systems (operate on bunch time scales,required for luminosity)
• Automatic correction of spin alignment as well?
Moritz Beckmann LC-Forum July 14, 2011 9/ 16
Static Misalignments (uncorrected)
Now: elements misaligned
• Random shifts in x and y for each element (some splitted!)
• Gaussian-distributed random numbers, σx ,y = 5 µmσx ,y = 50 nm in final focus region (0-50m in front of IP)
• Plots shows three exemplary samples
• Ignore collimators (beam loss)
distance from IP [m]-1680 -1660 -1640 -1620
lon
g. p
ola
riza
tio
n
0.6
0.7
0.8
UP
distance from IP [m]0 20 40 60 80 100 120 140
0.6
0.7
0.8
IP DP
not misaligned misaligned
UP/DP: up-/downstream polarimeter
Moritz Beckmann LC-Forum July 14, 2011 10/ 16
Static Misalignments (uncorrected)
, beam axis)bunch
p angle(≈>/(250 GeV) t
<p0 0.001 0.002 0.003 0.004
lon
git
ud
inal
po
lari
zati
on
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
+1)γ(a⋅precession
IP
UP
DP
• Same misalignments as before (σx ,y = 5 µm)
• Deviation from dashed line still under investigation
Moritz Beckmann LC-Forum July 14, 2011 11/ 16
Static Misalignments (corrected)
, beam axis)bunch
p angle(≈>/(250 GeV) t
<p0 0.5 1 1.5 2 2.5 3 3.5 4
-610×
lon
git
ud
inal
po
lari
zati
on
0.77
0.775
0.78
0.785
0.79
0.795
0.8
+1)γ(a⋅precession
IP
UP
DP
• Now: correct orbit in front of UP and at IP to < pt >= 0
• Even perfect orbit correction does not fix polarization at IP
Moritz Beckmann LC-Forum July 14, 2011 12/ 16
Static Misalignments (corrected)
longitudinal polarization at IP0.79 0.792 0.794 0.796 0.798 0.8
lon
git
ud
inal
po
lari
zati
on
at
UP
0.797
0.7975
0.798
0.7985
0.799
0.7995
0.8
y=x 0.1%±
968 of 1000 entries
longitudinal polarization at IP0.79 0.792 0.794 0.796 0.798 0.8
lon
git
ud
inal
po
lari
zati
on
at
DP
0.797
0.7975
0.798
0.7985
0.799
0.7995
0.8
y=x 0.1%±
968 of 1000 entries
hzpol_UPIPEntries 1000Mean 1.003RMS 0.003915Underflow 0Overflow 0
pol(UP) / pol(IP)0.95 1 1.05 1.10
50
100
150
200
250
300
350
Entries 1000Mean 1.003RMS 0.003915
hzpol_DPIPEntries 1000Mean 1.002RMS 0.003945Underflow 0Overflow 0
pol(DP) / pol(IP)0.95 1 1.05 1.10
50
100
150
200
250
300
Entries 1000Mean 1.002RMS 0.003945
Moritz Beckmann LC-Forum July 14, 2011 13/ 16
Static Misalignments (corrected)
longitudinal polarization at IP0.79 0.792 0.794 0.796 0.798 0.8
lon
git
ud
inal
po
lari
zati
on
at
UP
0.797
0.7975
0.798
0.7985
0.799
0.7995
0.8
y=x 0.1%±
968 of 1000 entries
longitudinal polarization at IP0.79 0.792 0.794 0.796 0.798 0.8
lon
git
ud
inal
po
lari
zati
on
at
DP
0.797
0.7975
0.798
0.7985
0.799
0.7995
0.8
y=x 0.1%±
968 of 1000 entries
hzpol_UPIPEntries 1000Mean 1.003RMS 0.003915Underflow 0Overflow 0
pol(UP) / pol(IP)0.95 1 1.05 1.10
50
100
150
200
250
300
350
Entries 1000Mean 1.003RMS 0.003915
hzpol_DPIPEntries 1000Mean 1.002RMS 0.003945Underflow 0Overflow 0
pol(DP) / pol(IP)0.95 1 1.05 1.10
50
100
150
200
250
300
Entries 1000Mean 1.002RMS 0.003945
Moritz Beckmann LC-Forum July 14, 2011 13/ 16
Summary
• A spin tracking framework for high energy linear colliders hasbeen set up
• ILC: understanding of polarization to permille-level required
• Implemented spin tracking through misaligned elements andhigher-order magnets
• Polarization in presence of misalignments: deviation fromsimple spin precession → investigate
• Assuring same beam angles at polarimeters and IP might notbe enough to fulfill polarimetry precision requirements
Moritz Beckmann LC-Forum July 14, 2011 14/ 16
Outlook: Other To-Do’s
• Insert missing beamline elements:• Detector magnets• Crab cavities & travelling focus (to enhance luminosity)
• Simulate collision effects (GP++/CAIN):
• Deflection (∼ 10−4 rad) fromcolliding bunch (T-BMT)
• Spin flip by emission ofbremsstrahlung (Sokolov-Ternov)
Moritz Beckmann LC-Forum July 14, 2011 15/ 16
Thanks for your attention!
Thanks for support and useful discussions to:
• David Sagan (Cornell)
• Deepa Angal-Kalinin (Daresbury)
• Anthony Hartin (DESY)
• Andrei Seryi (JAI)
• Kenneth Moffeit, Yuri Nosochkov, Michael Woods (SLAC)
• Jeff Smith (formerly SLAC)
Moritz Beckmann LC-Forum July 14, 2011 16/ 16
Upstream Polarimeter Chicane
• Constant magnetic field
• Dispersion (depending on beam energy): 1-11 cm
• Compton scattering: ∼ 1000 electrons per bunch
• Energy distribution → spatial distribution
• Cherenkov gas detector counts electrons per channel
Moritz Beckmann LC-Forum July 14, 2011 18/ 16
Idealized Lattice
, beam axis)bunch
p angle(≈>/(250 GeV) t
<p0 0.5 1 1.5 2 2.5 3 3.5 4
-610×
lon
git
ud
inal
po
lari
zati
on
0.77
0.775
0.78
0.785
0.79
0.795
0.8
+1)γ(a⋅precession
IP
UP
DP
Moritz Beckmann LC-Forum July 14, 2011 19/ 16
Idealized Lattice
longitudinal polarization at IP0.79 0.792 0.794 0.796 0.798 0.8
lon
git
ud
inal
po
lari
zati
on
at
UP
0.797
0.7975
0.798
0.7985
0.799
0.7995
0.8
y=x 0.1%±
1000 of 1000 entries
longitudinal polarization at IP0.79 0.792 0.794 0.796 0.798 0.8
lon
git
ud
inal
po
lari
zati
on
at
DP
0.797
0.7975
0.798
0.7985
0.799
0.7995
0.8
y=x 0.1%±
1000 of 1000 entries
hzpol_UPIPEntries 1000Mean 1.001RMS 4.76e-09Underflow 0Overflow 0
pol(UP) / pol(IP)0.95 1 1.05 1.10
200
400
600
800
1000Entries 1000Mean 1.001RMS 4.76e-09
hzpol_DPIPEntries 1000Mean 0.9994RMS 4.772e-09Underflow 0Overflow 0
pol(DP) / pol(IP)0.95 1 1.05 1.10
200
400
600
800
1000Entries 1000Mean 0.9994RMS 4.772e-09
Moritz Beckmann LC-Forum July 14, 2011 20/ 16