| ID |
Date |
Author |
Status |
Type |
Category |
Location |
Title |
|
83
|
Tue Nov 26 16:21:27 2019 |
Loïc Amoudry | Fixed | issue | vacuum | Optical room | Pneumatic valves |
The pneumatic valves are now plugged on the university air network.
The air valve is fully openned for the moment.
We still have to check if there is some minor leakage close to the pneumatic valve to improve the setup.
But it's not anymore an issue for the lock. |
|
82
|
Tue Nov 26 16:11:52 2019 |
Ronic Chiche | Fixed | issue | mechanics | Optical room | First Lock with 2nd satge of amplifier : Motor issue ? |
The 500 ms noise disapeared. We had to disable the "power save" mode of the smaract translation stage. AND turn OFF and ON the controler box.
| Ronic Chiche wrote: |
|
Global locking almost clean : tranmission and reflection are quite noiseless except the peaks at every 500ms.
During the amplifier 2nd stage lock, we experienced 2 strange behaviors :
- short "unlocks" every 500ms exactly all the time, during the whole lock process
- some PZT (in green on the picture) shift exactly synchronized with these "unlocks" (see the red circle).
these shifts are triggered by some OneFive motor move (Frep adjustment).
We tried to disconnect software activity (use the disconnect button on the software), to disconnect USB cable, to disconnect power supply of the motor controller box but none of these actions had an effect
=> still short unlocks every 500ms...
The amplifier 2nd stage seems to have small fan for the power supply... we can try to disconnect it.
We tried to turn on the 3rd stage which uses several fans for cooling the pump diodes... thus, one can see immediatly a big increasing in the PZT signal which tries to compensate the vibrations and quicly one loose the lock.
we have to think on how to suppress these vibrations.
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81
|
Fri Nov 22 17:56:56 2019 |
Ronic Chiche | Fixed | issue | lasers and optics | detectors and electronics | Optical room | 30Hz noise issue |
since some days, we observe the cavity is difficult to lock and a strange 30Hz noise has appeared on the PZT signal which normally compensate the phase noise difference between the cavity and the laser.
to test if the problem could come from the laser, we changed the OneFive laser for the Koheras but we have exactly the same problem, thus we concluded that the problem come from the cavity or from the feedback.
today, we borrowed an accelerometer measurement setup to Julien Bonis to test if we can see a clear noise at 30Hz from the seismic noise.
we placed to accelerometer directly on the top of the cavity but the spectrum we obtained do not show a clear noise line at 30Hz, only a small excess of noise in this region...
nothing which clearly indicate the cause of our problem.
yesterday, we changed the feedback setup in changing the PDH box from n°2 to N°3 without any change in the 30Hz noise line.
today, we also changed the feedback setup by introducing and amplifier of 100 just after the PDH box.
if noise is coupled after the amp we should be more immunized from it... but nothing changed again.
still looking for the origin of this problem... |
|
80
|
Thu Nov 21 11:37:13 2019 |
Loïc Amoudry | Fixed | info | lasers and optics | Optical room | Onefive Origami 33MHz specs |
Beam Size Onefive added
| Loïc Amoudry wrote: |
|
Power during ~20h, power after turn on, spectrum image and excel datas, polarisation and pulse length.
Powermeter measurments were done with a /10 filter.. 3 mW means 30 mW
Important: Onefive does not automatically locks after being turned on.
|
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| Attachment 1: beam_size.xlsx
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| Attachment 2: Beam_size_Onefive_33.rar
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79
|
Wed Nov 13 15:05:18 2019 |
Loïc Amoudry | Fixed | report | lasers and optics | Optical room | Amplifier output power |
| Loïc Amoudry wrote: |
|
The ouput power of the ThomX amplifier has been measured as a function of the 3rd stage pumps current (0A is 1st and 2nd stage turned on).
We measured the total power, the total power without the "donuts" pump signal dumped by an iris and the transmission of a dichroic mirror (for ref see image).
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| Attachment 1: courbedichro.PNG
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78
|
Wed Nov 13 14:44:56 2019 |
Loïc Amoudry | Fixed | report | lasers and optics | Optical room | Amplifier output power |
The ouput power of the ThomX amplifier has been measured as a function of the 3rd stage pumps current (0A is 1st and 2nd stage turned on).
We measured the total power, the total power without the "donuts" pump signal dumped by an iris and the transmission of a dichroic mirror (for ref see image). |
| Attachment 1: dichroic.PNG
|
 |
| Attachment 2: courbe.PNG
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| Attachment 3: power.xlsx
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77
|
Wed Nov 6 16:11:12 2019 |
Loïc Amoudry | Fixed | report | lasers and optics | Optical room | Spherical mirrors at closest position. FSR, finesse and beam size. |
The spherical mirrors are at the closest position to get a FSR ~=33.3435 MHz. Planar mirrors are at the largest position.
The finesse has been measured about 17 000.
Beam diameter (2*w) is ~= 4.6 mm x and y. |
| Attachment 1: data_finesse.isf
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| Attachment 2: fit_finesse_17000.png
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| Attachment 3: beamsize.PNG
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| Attachment 4: fit.PNG
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76
|
Tue Oct 22 09:10:45 2019 |
Loïc Amoudry | Fixed | report | lasers and optics | Optical room | First mode degeneracy on ThomX |
Yesterday, we've observed the first degeneracy on ThomX cavity at ~115 kW stored. The shape of the stored power on the oscilloscope is really close to what has been published in the D-shape mirror's paper ("tek0000" transmission in yellow, piezoelectric activator in green, error signal in blue).
This mode could be a 8.0 or 9.0.
We have also observed a change of the angle of the mode (the pictures "degenere", "degenere2" and "degenere3" were taken by order). The only changing parameters are the alignement and the length of the cavity.
The last thing we noticed is the shape of the mode which could not be an hermite-gauss mode (Bessel mode ?). |
| Attachment 1: degenere.PNG
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| Attachment 2: degenere2.PNG
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| Attachment 3: degenere3.PNG
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| Attachment 4: tek0000.png
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| Attachment 5: 100kWThomX.png
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75
|
Fri Oct 11 18:49:00 2019 |
Ronic Chiche | Fixed | info | detectors and electronics | Optical room | New locking scheme |
Before, the locking scheme was to produce an error signal with the PDH box, send its output to the electronic amplifier box and then to the laser EOM for the fast loop and to the Laselock input. The drawback was changing one loop gain, changes also the other loop gain.
Now, the locking scheme is the error signal coming from the PDH box is directly sent to the Laselock input and in a same time to the electronic amplifier box which is only connected to the laser EOM for the fast loop. then, one has the fast loop gain which can be changed with the electronic amplifier box, one has the slow loop gain which can be changed on the Laselock and if one needs to change global gain of both loops, one can move the PDH diffuser.
This scheme is currently used and locked the setup. |
|
74
|
Fri Oct 11 18:42:32 2019 |
Ronic Chiche | Fixed | issue | lasers and optics | detectors and electronics | Optical room | First Lock with 2nd satge of amplifier : Finesse issue ? |
First of all, we used and optical spectrometer to determine which proportion of pump and signal is in the injected beam.
the wavelength is THE SAME for the 2nd stage for the beam coming from the core or coming from the clad !
thus, it is impossible to use a spectrometer to obtain this proportion.
Thus, we made the assumption the pump beam (Sp) is unpolarized in contrary to the core beam (Sc) which is almost linearly polarized (Scp, Scs)
with a half waveplate and a PBS, we can define 2 cases in rotating the half waveplate at the output of the PBS :
maximum power : Scp + Sp/2 = a1
minimum power : Scs + Sp/2 = a2
The sum of both power a1 and a2 : a1+a2 = (Scp+Scs) + Sp is the total power of the beam before PBS.
The subtraction of power a1 and a2 : a1-a2 = Scp - Scs is independant of the pump power which can vary for example in opening an iris which normally block the most part of the pump beam.
if the core beam is perfectly linear, Scs=0 => a1-a2=Scp and Sp=2*a2
We did 2 measurements with a1=227mW, a2=67mW => Scp=160mW (Sp=134mW)
and with a1'=277mW, a2'=107mW => Scp=170mW (Sp'=214mW with a wider opened iris)
if these measurements and assumptions are correct, the real power injected to the cavity was 170mW (instead of 300mW).
with a coupling of 75% => Gain ~ 6.3k => Finesse ~ 19.7k !
to be confirmed...
| Ronic Chiche wrote: |
|
1st lock today with the second stage of the amplifier.
~ 300mW of injected power (but which proportion of the pump and of the signal ? => One must use a spectrometer to determine this proportion)
MAYBE the real injected power of the signal is lower => maybe the Finesse is higher !
Coupling ~ 75%
1.2 mW measured in transmission => ~800W inside the FP cavity
=> Gain ~ 3500 => Finesse ~ 11k !!!
Last Finesse measurement was about 19k ! :-(
|
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73
|
Thu Oct 10 18:03:10 2019 |
Ronic Chiche | Fixed | issue | mechanics | Optical room | First Lock with 2nd satge of amplifier : Motor issue ? |
Global locking almost clean : tranmission and reflection are quite noiseless except the peaks at every 500ms.
During the amplifier 2nd stage lock, we experienced 2 strange behaviors :
- short "unlocks" every 500ms exactly all the time, during the whole lock process
- some PZT (in green on the picture) shift exactly synchronized with these "unlocks" (see the red circle).
these shifts are triggered by some OneFive motor move (Frep adjustment).
We tried to disconnect software activity (use the disconnect button on the software), to disconnect USB cable, to disconnect power supply of the motor controller box but none of these actions had an effect
=> still short unlocks every 500ms...
The amplifier 2nd stage seems to have small fan for the power supply... we can try to disconnect it.
We tried to turn on the 3rd stage which uses several fans for cooling the pump diodes... thus, one can see immediatly a big increasing in the PZT signal which tries to compensate the vibrations and quicly one loose the lock.
we have to think on how to suppress these vibrations.
|
| Attachment 1: Image1.png
|
 |
|
72
|
Thu Oct 10 17:51:26 2019 |
Ronic Chiche | Fixed | issue | lasers and optics | detectors and electronics | Optical room | First Lock with 2nd satge of amplifier : Finesse issue ? |
1st lock today with the second stage of the amplifier.
~ 300mW of injected power (but which proportion of the pump and of the signal ? => One must use a spectrometer to determine this proportion)
MAYBE the real injected power of the signal is lower => maybe the Finesse is higher !
Coupling ~ 75%
1.2 mW measured in transmission => ~800W inside the FP cavity
=> Gain ~ 3500 => Finesse ~ 11k !!!
Last Finesse measurement was about 19k ! :-( |
|
71
|
Wed Oct 9 11:41:11 2019 |
Loïc Amoudry | Fixed | info | lasers and optics | Optical room | Onefive spectrum and CVBG spectrum |
The Onefive spectrum has shifted a little bit to lower lambda. It's still enough for the experiment (3mW injection of ampli intead of 1mW needed). |
| Attachment 1: 191008_spectrumbeforecvbg.PNG
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| Attachment 2: 191008_spectrumaftercvbg.PNG
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| Attachment 3: 191008_beamshapeaftercvbgthomx.PNG
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70
|
Wed Oct 9 10:16:24 2019 |
Loïc Amoudry | Fixed | info | lasers and optics | Optical room | Fiber injection and onefive output power |
Fiber injection is finished with the new ThomX stretching CVBG in double pass (+50% injection power compared to K-BOX CVBG in simple pass).
- Output Onefive: 27 mW
- After Onefive + lambda/2 + isolator: 25.8 mW
- After Onefive + lambda/2 + isolator + lambda/2 + PBS + CVBG*2 + PBS: 9.6 mW
- After injection into fiber and EOM (+all preceding): 3.2 mW
- Input 99% of the amplifier: 2.86 mW
> 660 mW on 1% photodiode DET100 @1Mohm |
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69
|
Wed Oct 9 10:10:01 2019 |
Loïc Amoudry | Fixed | info | lasers and optics | Optical room | Free Spectral Range (FSR) |
FSR is 33.347 MHz @1e-8 mbar
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68
|
Wed Oct 9 10:08:24 2019 |
Loïc Amoudry | Fixed | info | lasers and optics | Optical room | Improvement holder amplifier fiber |
We've added a clamp in the 3rd stage to prevent the pump fiber from moving and tilting (it was tilting to the left). |
| Attachment 1: 1.png
|
 |
| Attachment 2: 2.png
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67
|
Thu Oct 3 18:00:10 2019 |
Loïc Amoudry | Fixed | report | lasers and optics | Optical room | ThomX amplifier M2 |
The ThomX M2 has been measured between 1.5-1.6 for x and y |
| Attachment 1: Fit_matlab_M2.PNG
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66
|
Thu Oct 3 14:00:13 2019 |
Loïc Amoudry | Fixed | issue | cabling | Optical room | Electrical trouble (disjunction) |
The circuit breaker on ThomX cavity drops @1.5-1.8kW when we turn on 1/2nd stage of the amplifier or 3rd stage of the amplifier.
Amplifiers are now connected to K-BOX UPS.
We are buying a clamp ammeter for further investigations. |
|
65
|
Thu Oct 3 13:53:44 2019 |
Loïc Amoudry | Fixed | report | vacuum | Optical room | Cavity under vacuum |
The cavity is right now at 6.5e-8 mbar (turbo pumps on for 1 night and ionic pumps for 3h), primary pumps and turbo pumps are cut, ionic pump are on and the pressure level is still going down.
Therefore there aren't any big leak in the cavity and we can expect a final vacuum level close to e-9 mbar. |
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64
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Thu Oct 3 13:49:58 2019 |
Loïc Amoudry | Fixed | info | mechanics | Optical room | Pneumatic valves |
Frederic and Manu from vacuum group came this morning to fix again the pneumatic valves which had a leak again. |