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Entry   Mirror's installed, posted by Loïc Amoudry at Optical room about lasers and optics 

The initial 400kW SBOX mirrors which have been cleaned ont 28th of november have been installed this morning on the SBOX.

Entry   Mirror's cleaning, posted by Loïc Amoudry at Optical room about lasers and optics resume_M3.PNGresume_M1_M2_M4.PNG

XPS has been proceeded on the 400kW SBOX mirrors M3 and M4 (the initial cavity spherical mirrors) in frebruary 2019. Deposited a lot of particles on these mirrors.
All the mirrors received a Infrared spectroscopy the 12th of november 2019. Deposited glue on the non-reflective face (was used to hold them).
15th of november (2019): The four 400kW SBOX mirror's have been cleaned with aceton and isopropanol.
28th of november (2019): The four 400kW SBOX mirror's have been cleaned with spin coater.

Summary:

Aceton and isopropanol removed most of the particles and all the glue. But it let some traces on the mirror surface on all the mirrors (so there is some kind of grease on the surfaces).
Spin coater removes all the traces.

See pictures. On all the first images, we also see the dust which is on the non reflective face through the mirror. On M3 and M4 there is still the "glue" on the non reflective face on their frst images + refletive faces very dirty because of XPS.

Entry   AFM+ InfraRed spectroscopy (IR spectro) has been performed, posted by Loïc Amoudry at Other about lasers and optics 191113_AFMetspecIR-miroirs_SBOX.pdf

AFM+ InfraRed spectroscopy (IR spectro) has been performed on 400kW S-BOX mirrors.

Seems that XPS made M3 and M4 dirty, but M1 have also ome dust. M2 seems clean, further AFM experiment should show that it is as clean as M1.

Entry   Meeting with LMA people, AFM, posted by Loïc Amoudry at Other about lasers and optics POINT_SUR_LES_MIROIRS.pptx

30/01/19 - The following powerpoint shows the results discussed with LMA people.

What came out from the discussion is:

- Their cleaning method uses demineralized water drop on a spinner. It is probably the explanation of the circular traces on the mirror's surfaces but we still don't know what is this deposit (XPS is running out on 2 of this mirrors at this time).

-  According to their point of view, the spots could come from the coating deposition technique and are "normal". No real explaination, should not come from the substrat which is ultra-polished but can come from some clustering in the coating.

We gave them 2 of the mirrors so they can check if it is possible to clean them. They'll also do a measurement of the mirror's topology.

Entry   AFM performed on S-BOX mirrors, posted by Loïc Amoudry at Other about lasers and optics Image3.jpgImage4.jpg

29/02/19 - AFM has shown that spots on mirror's surfaces are bumps and not holes.

Entry   Impacts on mirror's surface, posted by Loïc Amoudry at Optical room about lasers and optics 18_M1reflectiveface2x_compressed.jpg

All the mirrors show impacts on there surface (some of them do not show deposit). Does it come from experiments or fabrication ? Are these holes or bumps ?

Entry   Deposit on S-box mirrors after return from LMA, posted by Loïc Amoudry at Optical room about lasers and optics 28_M2ReflectiveBeforeCleaning_compressed.jpg29_M2ReflectiveAfter1stCleanPaper_compressed.jpg

Cleaning on dirty surface shows something is deposited on the surface. Cleaning displaces and removes part of the deposit.

Entry   Mirrors features, come back from LMA, posted by Loïc Amoudry at Optical room about lasers and optics 181201_caracteristiques_miroirs.PNG20181207_155704_resized.jpg20181207_155726_resized.jpg

Mirrors arrived today from LMA. Their features are damaged.

Photos avant ou après nettoyage, pas clair dans le mail de Laurent : 

"J'ai commencé à nettoyer M1 et M2 avec notr methode habituelle et je me suis aperçu que sur la partie centrale (en gros taille de ton faisceau j'ai l'impression) que des choses apparaissaient (voir photo)
Si bien que la diffusion n'a pas évolué dans le bon sens (diminution) voir empiré pour M1. J'ai donc arrêter de les nettoyer !!!
J'ai regardé les faces arrières des miroirs avant nettoyage et j'ai pu voir ce que tu vois sur la photo même au centre. Je sais pas de quoi cela peut venir.
Une chose est sûre le coating IBS a été altéré par je ne sais quoi dans ta manip provoquant cette dégradation dès qu'on y touche. L'interaction avec les faisceaux d'eélectrons n'avait jamais altéré les miroirs sur l'expértience DESY par exemple!!
Pour me rassurer, j'ai pris un miroir fait sur un micropoli qu'on a en stock et aucun pb lors du nettoyage (on peut penser à tout)"
 

 

Entry   Mirrors cleaning, posted by Loïc Amoudry at Optical room about lasers and optics 

The new mirrors didn't give expected results. Then the 4 old mirrors have been sent to LMA on 12/11/18 for a cleaning and caracterization before and after cleaning. Also asked for a diffusion/absorption map on the mirrors if possible. They didn't really answered on what will they do. 
Received on 13/11/18 by LMA.

Entry   First run with spare mirrors, posted by Loïc Amoudry at Optical room about lasers and optics Plot_power_and_gain_vs_all.JPGpowerup.xlsx
I (A) Trans (mW) Coupling (%) Pin (W) Gain
0 4 70 0.37 4982
2 58 80 5.2 5140
4 180 75 16.1 5152
6 270 63 27.3 4558
8 340 60 36.7 4269

 

Entry   M1 transmission measurement, posted by Loïc Amoudry at Optical room about lasers and optics 

Center of M1:

I (A) Input power (mW) Transmitted power (mW) Transmission (ppm)
0 78 0.01477 189
4 16500 3.2 194
    Reply   M1 transmission measurement, posted by Loïc Amoudry at Optical room about lasers and optics 

At different positions, transmission give 194, 193, 208, 200 ppm?

Loïc Amoudry wrote:

Center of M1:

I (A) Input power (mW) Transmitted power (mW) Transmission (ppm)
0 78 0.01477 189
4 16500 3.2 194

 

Entry   M4 transmission measurement, posted by Loïc Amoudry at Optical room about lasers and optics 

The kept transmission for M4 is 2.17 ppm. Which is the value measured after alignement (center of the mirror).

These measurements have been taken before alignement.

I (A) Input power (mW) Transmitted power after window (mW) Transmission (ppm)
0 74.3 195.2e-6 2.63
0 73.5 212.8e-6 2.89
0 52.4 151e-6 2.88
6 28 400 72e-3 2.54

High dependence against the position. Few measurement several mm away from the center each one at different position give 194, 193, 208, 200 ppm.

    Reply   M4 transmission measurement, posted by Loïc Amoudry at Optical room about lasers and optics 
Loïc Amoudry wrote:

The kept transmission for M4 is 2.17 ppm. Which is the value measured after alignement (center of the mirror).

These measurements have been taken before alignement.

I (A) Input power (mW) Transmitted power after window (mW) Transmission (ppm)
0 74.3 195.2e-6 2.63
0 73.5 212.8e-6 2.89
0 52.4 151e-6 2.88
6 28 400 72e-3 2.54

High dependence against the position. Few measurement several mm away from the center each one at different position give 2.86, 2.68, 2.93, 3.01, 3.06, 3.35 ppm.

 

Entry   Change of the 3 ULE mirrors by 3 spare ULE mirrors, posted by Loïc Amoudry at Optical room about lasers and optics Miroirs_à_1031_nm-ThomX_-_décembre2017.pdfvacuum.isf

First finesse measurement 20 266, FSR 133.351 MHz under vacuum

Entry   Finesse vs power by difference between main and second resonance, posted by Loïc Amoudry at Optical room about lasers and optics CrossSecondaryResonance.mGetCavity.m

Measurements show that ratio decrease versus power. BUT, the second resonance measurement induce lower power in the cavity so the ratio is not directly true.

Also, simulation of the main/second resonance power by Pierre's simulation has shown ratio ~50, ~47.6 and 43.5 respectively for 0A, 2A and 4A.

I (A) Main resonance (mW) Second resonance (mW) Ratio
0 8.07 0.416 19.4
2 121 6.77 17.9
4 324 20.2 16

 

    Reply   Finesse vs power by difference between main and second resonance, posted by Loïc Amoudry at Optical room about lasers and optics 

Measurement on 24/10/18

Loïc Amoudry wrote:

Measurements show that ratio decrease versus power. BUT, the second resonance measurement induce lower power in the cavity so the ratio is not directly true.

Also, simulation of the main/second resonance power by Pierre's simulation has shown ratio ~50, ~47.6 and 43.5 respectively for 0A, 2A and 4A.

I (A) Main resonance (mW) Second resonance (mW) Ratio
0 8.07 0.416 19.4
2 121 6.77 17.9
4 324 20.2 16

 

 

    Reply   Finesse vs power by difference between main and second resonance, posted by Loïc Amoudry at Optical room about lasers and optics 

Measurement on 25/10/2018

Loïc Amoudry wrote:

Measurements show that ratio decrease versus power. BUT, the second resonance measurement induce lower power in the cavity so the ratio is not directly true.

Also, simulation of the main/second resonance power by Pierre's simulation has shown ratio ~50, ~47.6 and 43.5 respectively for 0A, 2A and 4A.

I (A) Main resonance (mW) Second resonance (mW) Ratio
0 8.07 0.416 19.4
2 121 6.77 17.9
4 324 20.2 16

 

 

Entry   Polarization frequency, posted by Loïc Amoudry at Optical room about lasers and optics 

Check of the frequency of the onefive locked on each polarization of the cavity (tilt a waveplate by 45°).

Frequency repetition rate : 133.335 MHz on spectrum analyzer for both polarization locked.

    Reply   Polarization frequency, posted by Loïc Amoudry at Optical room about lasers and optics 

Measurement on 30/10/18.

Loïc Amoudry wrote:

Check of the frequency of the onefive locked on each polarization of the cavity (tilt a waveplate by 45°).

Frequency repetition rate : 133.335 MHz on spectrum analyzer for both polarization locked.

 

Entry   Power measurement with D-shape, posted by Loïc Amoudry at Optical room about mechanics | lasers and optics 

Measurements of lot of points with D-shape mirrors well positionned.

Power not optimized to the best but almost. (@4A could have 350 mW).

I (A) Ptrans (mW)  Coupling (%)

0

8 62
1 18 67
1.3 43 72
1.6 76 72
1.9 112 72
2.2 145 72
2.5 177 72
2.8 217 72
3.1 253 72
3.4 281 72
3.7 300 72
4 323 71
4.3 249 71
4.6 379 68
4.9 402 68
5.2 417 67
5.5 435 67
5.8 441 65

 

Entry   Beam size vs D-shape position, posted by Loïc Amoudry at Optical room about lasers and optics 181018_4A_no_cut.PNG

Measurement done on 18/10/18.

At high power, the shape of the 0.0 mode does not change. The D-shape only generate losses in the cavity. Then the power stored in the cavity decrease. As with this configuration, the cavity beam size decrease when power increase, the beam size decreased.

Measurements done @4A on 3rd stage.

x (um) y (um) Picomotors displacement (um) Transmission power (mW)
1820 2013 0 337
1820 2013 200 330
1925 2029 400 306
1936 2090 600 245
2117 2249 800 125
2260 2392 1000 17

Then we get the D-shape away from the beam to not cut it and decreased the amplifier power to validate the beam size at a known value. So the power as been decreased to 2A (= 125 mW in trans) and the beam size was x=2079 y=2255, similar to the 125 mW with D-shape mirrors values.

    Reply   Beam size vs D-shape position, posted by Loïc Amoudry at Optical room about lasers and optics size_vs_position_and_power.JPG

Matlab code for size vs position and power : 

clear all
close all

x = [1820 1820 1925 1936 2117 2260];
y = [2013 2013 2029 2090 2249 2392];
Position = [0 0.2 0.4 0.6 0.8 1];
Trans = [337 330 306 245 128 17]

hold on
[ax,h1,h2] = plotyy(Position,x,Position,Trans)
set(get(ax(1), 'Ylabel'), 'String', 'Beam diameter (um)');
set(get(ax(2), 'Ylabel'), 'String', 'Transmitted power (mW)');
xlabel('Position of the D-shape (mm)')
plot(Position,y,'g')
hold off

Loïc Amoudry wrote:

Measurement done on 18/10/18.

At high power, the shape of the 0.0 mode does not change. The D-shape only generate losses in the cavity. Then the power stored in the cavity decrease. As with this configuration, the cavity beam size decrease when power increase, the beam size decreased.

Measurements done @4A on 3rd stage.

x (um) y (um) Picomotors displacement (um) Transmission power (mW)
1820 2013 0 337
1820 2013 200 330
1925 2029 400 306
1936 2090 600 245
2117 2249 800 125
2260 2392 1000 17

Then we get the D-shape away from the beam to not cut it and decreased the amplifier power to validate the beam size at a known value. So the power as been decreased to 2A (= 125 mW in trans) and the beam size was x=2079 y=2255, similar to the 125 mW with D-shape mirrors values.

 

Entry   Transmission vs D-shape position at different powe, posted by Loïc Amoudry at Optical room about lasers and optics Plot_matlab.JPGmotors.xlsxPower_stored_vs_Dshape_mirrors_position.m

Measurements have been done on 18/10/18.

Datas are on excel file, also matlab file.

Entry   Motors for D-shaped mirrors, posted by Loïc Amoudry at Optical room about mechanics | lasers and optics tek00000.pngtek0000CH1.isftek0000CH2.isftek0000CH3.isftek0000CH4.isf

Motors have been installed on 16/10/18. No problem with them.

Effect of the motors tested on 17/10/18. No improvement. But they give the possibility to perfectly cut HOM or let them go through as show the following picture of a 2.2 mode at ~340 mW in trans and 70% coupling @4A.

Entry   Record power-up, posted by Loïc Amoudry at Optical room about lasers and optics 

Measurement made on 03/10/18 (nothing has been done since there).

Stable power in the cavity of 225 kW.

3rd stage current Transmission (mW) Pin (W)
0 8 0.37
2   5.3
2.2 145 6.4
3   10.7
4 350 16.1
5   21.8
6   27.3
7   32
8   36.7
8.5 640 39.1

 

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