Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R.,...
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Transcript of Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R.,...
![Page 1: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/1.jpg)
Nonplanar Cavity Construction and
Locking Technique for High Finesse Cavity
Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F.
Laboratoire de l’Accélérateur Linéaire, Orsay, France
![Page 2: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/2.jpg)
Outline
• Why a nonplanar cavity 1.Compact size(mechanical stability, vacuum)
2.No reverse beam
3.Easy adapt to the different frequencies
4. Elliptic particle beam astigmatic eigen mode of the cavity = nonplanar cavity
• Cavity for ATF (KEK)1. Mode structure2. Construction
• Requirements for laser to cavity tight locking - requirements for electronics
- requirements for actuators
• Digital Feedback for locking a pulse laser to the optical cavity
![Page 3: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/3.jpg)
Nonplanar cavity
• Why a nonplanar cavity 1.Compact size(mechanical stability, vacuum)
2.No reverse beam
3.Easy adapt to the different frequencies
4. Elliptic particle beam
astigmatic eigen mode of the cavity = nonplanar cavity
Eigen modes of such cavities =
gaussian beam with general astigmatism
e
ph
IP
![Page 4: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/4.jpg)
Optical scheme of the nonplanar cavity
2 plan mirrors
2 spherical mirrors
WAIST
.
Injection laser
e-Interaction
point
Electron pipe
![Page 5: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/5.jpg)
Fundamental mode of the nonplanar cavity
Distance between the curve mirrors: 502.8mm
Transverse scale: 0.1mm =
Longitudinal stepbetween two successive images : ~ 8mm
![Page 6: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/6.jpg)
Fundamental mode of the nonplanar cavitydictorted by abberations
Distance between the curve mirrors: 502mm
Transverse scale : 0.1mm =
Longitudinal stepbetween two successive images: ~ 8mm
![Page 7: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/7.jpg)
Cavity construction for ATF
Compact construction operated under high vacuum and remotely adjusted
![Page 8: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/8.jpg)
PZT
Cavity mirrors actuators
θx
θy
PZT
Flexible support
Mirror
Step motorin vacuum housing
![Page 9: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/9.jpg)
Pulse laser locking to the optical cavity
• Principle : coherent combinig of the successive laser pulses inside the optical cavity :
--> mutual coherence of pulse laser <-> cavity
--> two parameters locking
carrier
envelope
Fabry-Perot Cavity
FSR
Laser spectrum
Cavity eigen modes
CEREPn ffn
2_CCEFP
n nFSR
![Page 10: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/10.jpg)
Pulse laser – cavity locking through the one-parameter
F_ce lockingF_rep ramping
F_rep lockingF_ce ramping
Two parameters have to be locked
Requirements on the actuators: 1.big dynamic range (ramping) 2. min noise (tight lock)
Two actuators for each paramaters: one for the ramping another for locking
-1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 10
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
PHIce/(2 pi) (without unit)
no
rma
lized
tra
ns
mit
ted
po
wer
Fabry-Perot cavity transmision power sensitivity over PHIce, Tau = 2ps
Requirements on the electronics: noise level inside the bandwidth of the actuators smaller than noise necessary for the tight lock.
L
F
f
One-parameter locking
F-cavity finessefL- laser frequency
![Page 11: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/11.jpg)
Scheme of the pulse laser locking on the optical cavity
grep
vf
L
gceo
v vf
1. Ramping frep – motor M1
2. Locking frep -PZT
1. Ramping fceo – starter (wedges)
2. Locking fceo – AOM1+AOM2
PumpLaser
U=0U=δ
![Page 12: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/12.jpg)
Digital Feedback (1)
PH REFLEXION
DPDHDPDH
command
command
command
PH TRANS
DDSDDS
ADC
ADC
ADC
DPDHDPDH
FPGA
PZT
AOM
VHS-ADAC
EOM
DAC
DAC
DAC
DAC
PH REFLEXION
![Page 13: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/13.jpg)
Digital feedback (2)
1. 2 inputs + 4 outputs parameters = MIMO
2. Nonstationary response of F-P cavity
3. Nonlinear reaction of the feedback system: ramping + triggering + filtering (linear and nonlinear)
4. Simple communication with the another digital systems
Lyrtech: VHS-ADAC8 inputs - 8 outputsparallel ADC, DAC, 14bits Latency : 60ns (ADC) + (0.3-1)µs + 40ns (DAC)
![Page 14: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/14.jpg)
Frep phase noise
PDH voltage noise power densityin closed loop Sv(f)
Estimation ofPhase noise in closed loop
and in open loop
ΔFrep RMS ~ 1 mHz (@ f<100kHz) in CL
For coupling 90% of the powerOne needs ΔFrep RMS ~ 0.1 mHz
Detection noise floorPDH noise floor
Unity gain frequency ~ 10 kHz
0 0
0
( )6
0.16
Frepf n n Frep
FrepFrep mHz
n
F
F
![Page 15: Nonplanar Cavity Construction and Locking Technique for High Finesse Cavity Soskov V., Chiche R., Cizeron R., Jehanno D., Zomer F. Laboratoire de l’Accélérateur.](https://reader030.fdocuments.in/reader030/viewer/2022032414/56649eec5503460f94bfd94f/html5/thumbnails/15.jpg)
Frep frequency noise
101
102
103
104
105
106
107
108
-80
-60
-40
-20
0
20
40
60
Frequency (Hz)
Nois
e P
ow
er
(dB
c/H
z)
100
102
104
106
108
10-1
100
101
102
103
104
105
Frequency (Hz)
Estimation of theFrequency noise power density
of the carrier in closed loop
Estimation of theIntegrated Frequency noise power
of the carrier in closed loop
0( ) 5006
Frepf n Hz
F
Detectionnoise floor
~5 kHz