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Entry   New mirrors batch informations, posted by Ronic Chiche at ThomX igloo about lasers and optics miroirs_puma_2022_thomx_Kbox.docxMiroirs_à_1031_nm-ThomX_-_KBox_Mars_2023.pdfRecap_miroirs_KBOX_et_THOMX.xlsx

the 2 files describe the specfications for the 16 mirrors ordered (4 for ThomX + spare, 4 for SBOX + spare) and the measurements made by the LMA.

I add also a 3rd file in which all the "special' mirrors are referenced.

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   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+ 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   Cavity polarization states (Koheras), Finesse of 2 polarization states, posted by Loïc Amoudry at Optical room about lasers and optics Finesse_higher.isfFinesse_lower.isfThe2polarizations_states_direct_trans.isfThe2polarizations_states_direct_trans.png

Measurments of Finesse with the 2 polarization states, let's call them H (higher) and L (lower): 24500 for the H and 23500 for the L.

We checked the polarization states in transmission of the FP cavity after a PBS. The H was stronger in PBS trans and the L stronger in PBS ref.

We measured the power in reflection of the PBS and added a half WP that we aligned with the PBS polarization. Then, to get the maximum power we had to tilt the half WP of 22° for the H and 18° for the L.

Finally we checked the extinction through half WP and PBS for H and L. 

- For H : max 75 mW min 5 mW. Ratio 6.66%

- For L : max 70 mW min 4 mW. Ratio 5.7%

Right after Koheras : max 3.5 mW min 47 uW. Ratio 1.3%

 

Entry   Phase measurement with HASO, posted by Loïc Amoudry at Optical room about lasers and optics 180928_M2_0A.has1801001_input_0A.has180928_M2_trans_0A.txt

2 measurement.

First one locked, in transmission of M2 with 2nd stage 0A.Total 89 cm from the big waist (planar mirrors). 2 wedges used.

Second one at input beam with the same power. Datas taken at the same equivalent position than the first one. 3 wedges used.

    Reply   Phase measurement with HASO, posted by Loïc Amoudry at Optical room about lasers and optics 8x

* Loic has to fix the number of files (3) regarding the number of measurements (2)

* splitted Intensity and phase HASO files

* image for each file

Loïc Amoudry wrote:

2 measurement.

First one locked, in transmission of M2 with 2nd stage 0A.Total 89 cm from the big waist (planar mirrors). 2 wedges used.

Second one at input beam with the same power. Datas taken at the same equivalent position than the first one. 3 wedges used.

 

    Reply   Phase measurement with HASO, posted by Loïc Amoudry at Optical room about lasers and optics 

with just intensity, the coupling is 98%, and with phase, x direction coupling is 95%, y direction 97%, so the telescope is good.

Loïc Amoudry wrote:

* Loic has to fix the number of files (3) regarding the number of measurements (2)

* splitted Intensity and phase HASO files

* image for each file

Loïc Amoudry wrote:

2 measurement.

First one locked, in transmission of M2 with 2nd stage 0A.Total 89 cm from the big waist (planar mirrors). 2 wedges used.

Second one at input beam with the same power. Datas taken at the same equivalent position than the first one. 3 wedges used.

 

 

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

Optimization of the polarization has been made the 03/10/18. Checked in reflection of the cavity in reflection&transmission of a PBS, locked and unlocked. Only with 2nd stage.

Ratio values are reflection of PBS divided by transmission or the opposite.

  Unlock value Ratio min/max Lock value Ratio min/max
No optimization        
Reflection 1.21 X 3.89 X
Transmission 14.3 8.5 % 3.1 80 %
Only Lambda/2        
Reflection 4.4 X 2.91 X
Transmission 11 40 % 2.79 96 %
2xLambda/2 + 1Lambda/4        
Reflection 8.3 X 3.4 X
Transmission 6.8 82 % 2.2 65 %
Same + PID optimization        
Reflection 9 X 3.35 X
Transmission 5.76 64 %  2 60 %

 

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

 

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   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   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   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   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

 

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.

 

    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

 

 

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