1 la electronics meeting, cascina, 25.01.2006 virgo alignment system overview ● linear alignment...
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1 LA electronics meeting, Cascina, 25.01.2006
Virgo alignment systemoverview
● Linear Alignment principle● Optical configuration
● Present situation● Foreseen developments
2 LA electronics meeting, Cascina, 25.01.2006
The VIRGO Interferometer
N
W
EOM
Task of the alignment system:Keep 6 mirrors and input beam aligned
5 output beams for obtaining error signals
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Basics of error signal retrieval
Phase modulation of input beam
Demodulation of photodiode signals at different output beams=> longitudinal error signals
Quadrant diodes in output beams=> Alignment information (differential wavefront sensing)
Anderson-Giordano technique2 quadrant diodes after arm cavities
Quadrant diode
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Can have 1 normal diode and 2 quadrant diodes at each output port
Detection
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Optimized alignment noise budget
Maximized powerOptimized mirror centering
(0.2 mm)
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Present situation
Frascati group is leaving VirgoSince 01/2006
Frascati’s responsibilitiesOriginal design of alignment system
Strategy, optics, prototype experiments, …
Design & realization of electronics
ProblemContinue support for alignment electronicsMake new modules / spare modulesContinue development for new requirements
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Developments
Present developmentsMore modules needed
Installation of 9th quadrant diode (maybe 10th)Spares needed
New Annecy local oscillator boards, compatible with alignmentPhase shifters for standard photodiodes
Possible developmentsSubstitute Si diodes with InGaAs diodes
Better quantum efficiencyLower bias voltage
=> higher power capability lower noise
Reduction of electronics noiseBetter preamplifier: 5 pA/rtHz -> 1.6 pA/rtHz (?)DC signals: pre-amplification / pre-shaping
Fast quadrant centering system(Napoli is working on that)LA noise limits sensibility (especially at low frequ.)
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Quadrant photodiode
•type EG&G YAG 444
•sensitivity = 0.45 A/W
•DC power = 3 mWmax
•transimpedance = 2 k•Bias voltage = 180 V
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QD electronics
dem
odul
ator
phas
e sh
ifte
r
Quadrant diode box
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Scheme of LA electronics
ADC noisePreamp. noise
Shot noise
Low-pass filter
AC: Gain 200
DC: Gain 1
diff. sig.
non-diff.sig.
Non-optimal treatment of DC signalsdominated by ADC noise(but were not foreseen as error signals)
VMEQD box
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Noise measurements
after demodulator
quadrant diode AC output
Theoretical shot noise M. Mantovani
dem
odul
ator
gai
n
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C7 matrix
ThetaX PR BS NI NE WI WEB2_q1_DC 2.5 -4.5 -6.4 15B5_q1_DC 10B2_q1_ACp -24 9.41 17.9 5.38B1p_q1_ACp 0.052 -0.108 0.0375 1 0.0729B7_q1_ACq 0.042 -0.035 0.375 -0.027B7_q2_ACq 0.042 -0.035 0.375 -0.027B8_q1_ACp -0.25 0.65 0.052 0.071B8_q1_ACq -0.25 -0.65 -0.052 -0.071
ThetaY PR BS NI NE WI WEB2_q1_DC 1B5_q1_DC 10B1p_q1_ACq 1B7_q1_ACp 0.33 0.36B7_q2_ACp 0.68 0.36B7_q2_ACq -0.36 -0.36B8_q1_ACp -0.46 -1 -0.36B8_q2_ACp 1
ThetaX has undergone second diagonalization => mixing of all signals
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Total LA electronics noise (C7, calculated)
WE ty pure DC error signal => no extra noise vs. AC
WI under local controlSimulated WI LA curves for comparison
C7 noise not limited byLA electronics noise
(but: excess noise)