lock acquisition of the virgo citfmoriond.in2p3.fr/j03/transparencies/5_thursday/2...citf...
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Lock Acquisition ofthe Virgo CITF
Lisa BarsottiUniversity and INFN – PISA
on behalf of the on behalf of the VIRGO CollaborationVIRGO Collaboration
XXXVIII Rencontres de Moriond 27th March 2003
Summary
CITF
Lock acquisition problem
Lock acquisition strategy
Statistical approach about lock acquisition
CITF Configuration
0lPR
WI
NIBS
B1
B5
Simple Michelson
1l
2l
The CITF working conditions are:
resonance of the stored power in the RC
Michelson on the dark fringeTwo lengths must be
controlled
Two typical lengths:
• Recycling Cavity (RC) length:
• Dark Fringe (DF) length:2
llll 210r
++=21 lll −=∆
Lock Acquisition Problem
Frequencies below 4 Hz: seismic noise
Need of a control system in order to keep the ITF locked to the required interference conditions
Lock Acquisition Problem
Optical signals as correction signals sent to the mirrors by feedback
0l 1l
2l
PR
WI
NIBS
RC Correction signal
DF Correction Signal
B5B1
Lock Acquisition ProblemLimits on the mirrors speed which
can be controlled
Bandwidth grater than few hundreds Hz not feasible because of computational andantialiasing delay in the control chain
Limit on the maximum force applied related with noise considerations
Bandwidth of the Feedback
sm2.0~2Bv µλℑ< sm2~ m2
λF v MAX µℑ<
Maximum force applied
Finesse
Wavelength
Bandwidth
Maximum Force
m064.1 µλ=
Hz100B=
250=ℑ
mN40F max=
Lock Acquisition Problem
Mirrors speed out of the limits placed by the correction system
Energy transferred by actuators to the mirrors during lock acquisition trials
No local controls along optical axis
We need such a strategy to avoid these problems on the mirrors speed
Optical DampingIn order to reduce mirrors excitations (0.6 Hz resonance) and the time of lock acquisition we have studied the OPTICAL DAMPING, which allows to damp excited mirrors.
Low speeds are reached in few seconds
PR
WI
NIBS
Simple Michelson
WI excited
PR misaligned
Error signal: B1_quad
B1
PR
WI
NIBS
PR-NI Cavity
Error signal: B1_quad
B1
WI misaligned
PR excited
Example of optical damping
WI Correction
B1_DC
PR Mirror Misaligned
(Volt)
(a.u)
WI Velocity of the order of tens µm/s
optical damping
WI velocity reduced
to the order of µm/s
Lock Acquisition StrategyAsymmetric trigger on the stored intensity
Lock acquisition is tried only when the mirrors are near to the rightresonance (that is the fundamental mode of the stored intensity)
(s)
Opening
Closing
Volts Stored Power Trigger opening: about one half of the maximum power
Trigger closing: few % of the maximum power
Enlargement of the action time interval of the
feedback
Lock Acquisition StrategyLinearization of the error signals
In order to enlarge this action time interval of the feedback we should linearize the error signals
0=n
2=n 23=n
1=n
Search for RC error signal in the following form:
DCBphaseB
n_5_5
0=n
2=n 23=n
1=n
23_5_5
DCBphaseB
Best choice for RC error signal:
Lock Acquisition StrategyLinearization of the error signals
In order to enlarge this action time interval of the feedback we should linearize the error signals
Lock Acquisition StrategyLinearization of the error signals
(s)
a.u23_5
_5DCBphaseB
CITF Configuration(only-mirrors)
0l 1l2l
BS
WI
PR
NI
B5B1
23_5_5
DCBphaseB
DF Error signalquadB _1
RC Error signal
Example of a Lock Acquisition Event
Stored Power (B5_DC)
WI CorrectionPR correction
Output Power (B1_DC)
(s) (s)
(s)(s)
(Volt)(Volt)
(a.u) (a.u)
We have a lock acquisition algorithm
Following steps:
•Systematic study of locking attempts
• Computation of the efficiency
• Improvement of the efficiency
Algorithm efficiency
How can we improve the efficiency ?
Locking success is due essentially to the mirrors speed
Trigger on RC Speeds
Trigger on DF Speeds
Lock Algorithm Efficiency
0056.0897
5=
Data Analysis Results
897 failed attempts 5 locking successes
Data taking by locking and delocking the CITF – 1 hour of data
Looking for
2 independent signalswhich describe
the RC speed and the DF speed
•
DCBACpB
_5Pr__5Pr_
23RC Speed Trigger - TEST OF
Sweep on RC •
DCBACpB
_5Pr__5Pr_
23
(s)
(a.u)(Volt)
1
2
DCB _5Pr_
0.21 0.211 0.212 0.213 (s)
(s)
1
2
0
0.5 0.55 0.6
Sweep on DFDCB _5Pr_
(Volt)
0.5 0.55 0.6
0
50
100
(s)
•
DCBACpB
_5Pr__5Pr_
23(a.u)
4000
2000
0
0.2110.21 0.212 0.213
The difference between these values is about two order of magnitude
is a good trigger!•
DCBACpB
_5Pr__5Pr_
23
•
DCBACpB
_5Pr__5Pr_
23RC Speed Trigger - TEST OF
Trigger on the RC speedIf we place a trigger on the RC speed, how much does algorithm efficiency improve?
By seeing the 5 good events : 1.34 max RC Speed
Locking attempts with RC speed < 1.34 : 415
smµ
smµ
Efficiency with trigger
0120.0415
5=
Efficiency without trigger
0056.0897
5=
By simulation:(Volt)ACpB _5Pr_ DCB
ACpB_5Pr__5Pr_
23(a.u)
7~α
Final conditions on :v
smm
Fv
smBv
µλα
µλα
13~2
5.1~2
max
ℑ<
ℑ<
Analysis of Results
Now we are into the expected velocity
range!
DF Speed Trigger – TEST OF ACqpB _1Pr_ 3•
Sweep on RC
Sweep on DF
DCB _5Pr_
0.21 0.211 0.212 0.213 0.21 0.211 0.212 0.213
0.50 0.60 0.50 0.60
1
0
2
1
0
20.02
0
0.04
0
-0.02
-0.04
-2000
2000
(Volt)
(Volt) (A.u)
(A.u)
0.55 0.55
DCB _5Pr_
ACqpB _1Pr_ 3•
ACqpB _1Pr_ 3•
DF Speed Trigger – TEST OF ACqpB _1Pr_ 3•
The difference between these values is morethan two order of magnitude
is a good trigger!ACqpB _1Pr_ 3•
Combined triggersHow much does the efficiency improve if we place a
trigger on RC speed and a trigger on DF speed at the same time?
We consider as triggers threshold theMAX speeds of locking successes
Efficiency: 017.0~2975 Improvement
of a factor 3
Speeds Distribution
0 0.05 0.1 0.15 0.2 0.25 0.3
-4x100
5
10
15
20
25
30
35
40
Nent = 897Mean = 2.662e-06RMS = 3.02e-06
Nent = 897Mean = 2.662e-06RMS = 3.02e-06
(M/SEC)
RC Speed Distribution
0 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08 0.09 0.1
-4x100
5
10
15
20
25
Nent = 897
Mean = 8.987e-07RMS = 5.831e-07
Nent = 897
Mean = 8.987e-07RMS = 5.831e-07
(M/SEC)
DF Speed Distribution
Speeds Distribution
-0.2 -0.15 -0.1 -0.05 -0 0.05 0.1 0.15 0.2
-4x10-0.2
-0.15
-0.1
-0.05
-0
0.05
0.1
0.15
0.2-4x10 Nent = 897
Mean x = 6.532e-07
Mean y = 4.345e-08
RMS x = 3.972e-06
RMS y = 1.07e-06
Nent = 897
Mean x = 6.532e-07
Mean y = 4.345e-08
RMS x = 3.972e-06
RMS y = 1.07e-06
m/s RC Speed
DF
Spee
dm/s
ConclusionsDevelopment of the lock acquisition algorithm
(thanks to a full digital control system):
• asymmetric trigger
• linearization
• optical damping
Systematic study of the lock acquisition
Triggers on the speeds
Starting point for full VIRGO
• Lock Acquisition Simulation in progress