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A HighA High--Finesse Finesse FabryFabry--PPéérotrot Cavity for Hall ACavity for Hall A
Compton Compton PolarimetryPolarimetry
AbdurahimAbdurahim RakhmanRakhman
Department of Physics,Department of Physics, Syracuse University, Syracuse, NYSyracuse University, Syracuse, NY
HUGS 2008, Jefferson LabHUGS 2008, Jefferson Lab
June 20, 2008June 20, 2008
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IntroductionIntroductionPrinciple of Compton polarimetry
Compton polarimeter at Jefferson Lab
Hall A Compton polarimeter upgrade
Implementation of Implementation of FabryFabry--PPéérotrot cavitycavityCavity optics
Cavity resonance modes
Cavity locking
SummarySummary
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Polarized Electron SourcePolarized Electron Source
In a polarized beam, the spins point in a single direction. The accelerator at Jefferson Lab can produce two types of longitudinally polarized beam
Via polarized electron scattering, physicists gain insight into what physical processes are involved in an event. This technique is useful for many open research questions, such as:
Polarimetry, the measurement of the beam polarization, allows us to accurately interpret the data and control for errors.
Right-handed
Left-handedUnpolarized electrons
How densely are neutrons distributed in a heavy nucleus like lead ?Do strange quarks contribute to the physical properties of protons ?How is electrical charge distributed inside the neutron ?
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Principle of Compton Principle of Compton PolarimetryPolarimetry
σ +e- γ
σ −e- γ
E, E’ k, k’
><××== −+
−+
+−
thennnn APPA γexp
Measurable Theoretical Calculation
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Why optical cavity is chosenWhy optical cavity is chosen
<<1
Amplified by optical cavity: G
dzdxdyvL erel γρρ∫∫∫=
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6174 ft
55 ft
Compton Compton PolarimeterPolarimeter at Jefferson Labat Jefferson Lab
MøllerCompton
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Compton Compton PolarimeterPolarimeter at Jefferson Labat Jefferson Lab
Compton Int. Point
γ detector
e- detector Hall A
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Hall A Compton Hall A Compton PolarimeterPolarimeter UpgradeUpgrade
Twice the Analyzing power of present IR cavity, two-
fold increase in Figure-of-Merit
Improve accuracy of polarization experiments by providing 1% beam polarimetry
down to 1 GeV. High precision parity violating experiments (such as PREx) are
feasible with this upgrade.
High resolution silicon micro strips to improve tracking resolution
Improve systematic uncertainties experienced in the
counting method While preserving counting abilities
New Electron Detector :
New Photon Detector :
Green Fabry-Pérot Cavity :
Motivation:
Dynamic Range : 2 GeV ~ 6 GeV 0.8 GeV ~ 11 GeV
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Green Green FabryFabry--PPéérotrot CavityCavity
Wavelength 532 nm
Mirror Reflectivity 99.996266 %
Power 1,500 Watts
Gain 15,000
Q-factor 1.8 x 1011
Free Spectral Range 176 MHz
Cavity Band Width 3.12 kHz
Length 0.85 m
Mode CW, TEM00
CIP spot size (σ) 87 μm
Low power Green Laser -> High Finesse cavity -> Feedback to laser PZT to lock
Incident
Reflected
Circulation
Transmission
r1 r2
L
Mounting slot for a cavity mirror
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Optical SetupOptical Setup
Beam Position Monitoring Arm
Laser
Fabry-Pérot Cavity
Alignment Laser
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Cavity transverse modeCavity transverse mode
YX
Z
Z
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Cavity Mode MatchingCavity Mode Matching
● Laser mode (beam) should match the cavity resonator mode
● Beam waist at the center should match the natural waist of the cavity
● The amount of primary power actually amplified in the fundamental mode
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R=0.9
R=0.8
R=0.7
● Keep the cavity resonate forever
● It is very hard to stabilize the cavity length in nm level
Cavity ResonanceCavity Resonance
R=
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-1 -0.5 0 0.5 1
-1.5
-1
-0.5
0
0.5
1
1.5
Characteristic Signals of a Characteristic Signals of a FabryFabry--PPéérotrot CavityCavity
kHz
Reflected Intensity
Detuning Parameter
Phase
Reflection
Reflection Phase
Transmission
50100 0 50 100
• Detect phase of the resonance from reflected light
• Feedback to tunable element to stay “locked” to resonance
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Tunable Laser Beam Splitter
Cavity
Photo detector
Oscillator
Phase Shifter
MixerLow Pass Filter
PID-Regulator
0
near resonance
Pound-Drever-Hall Locking Scheme
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Cavity LockingCavity Locking
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SummarySummary
Low gain (G ~ 1,000) cavity locking has been accomplished
Working on design goal cavity (G ~ 15,000) locking
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Compton Lab ARC L312Compton Lab ARC L312
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