ID |
Date |
Author |
Type |
Category |
Subject |
380
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Fri Jun 21 11:47:30 2024 |
Liu | Update | Scripts/Programs | COMSOL simulation on alternative straightened heater elements design |
In the previous post, we saw that for the heater element design with straight edges in replacement of the current eight-element ring-like design, it provides the similar Gaussian-like irradiance profiles, but with smaller power delivery efficiencies, as shown in the plot. This turned out to result in similar but less prominent thermal effects.
They only differ from the original baseline design by a source power rescaling, however, as shown in the plot, where we see the power-rescaled irradiance profiles for the straight edge designs are close to that for the ring design. The resulting temperature profiles and thermal distortions are shown in plot and plot. The thermal effects for the 16 straight-edge design with renormalized source power for instance are strikingly similar to that for the original ring design.
An alternative straightened heater element design has also been investigated with COMSOL FEA simulation. As shown in the attached, in this new design each heater element component is cut with multiple straight edges but remains connected, shown in the same colors (green and red). In the example, four straight edges are cut from each of the four heater components (4x4=16 edges in total). There is no spacing between the neighboring edges from the same element component, but the edges from different components are separated by 2mm, as can be seen in the attached. This new N-in-one straight edge design offers similar irradiance compared to that for the evenly-spaced N-sided regular polygon straight edge design with the same number of edges, as shown in the plot. It however has fewer heater components, four in this case, which makes it easier to implement in assembly and wiring, and less vulnerable to electrical and thermal shorts with their fewer heater element pins. |
Attachment 1: rayIllu_side_new.png
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Attachment 2: rayIllu_full_new.png
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Attachment 3: Irradiance_profile.pdf
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Attachment 4: Irradiance_profile_norm.pdf
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Attachment 5: temp_profile.pdf
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Attachment 6: thermal_distortions.pdf
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375
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Mon Jun 10 14:52:38 2024 |
Tyler | Update | FLIR | CIT FROSTI Analysis Update |
[Tyler]
Upon further inspection, one adjustment was made to the FROSTI profile analysis: changing the transmission value of the ZnSe viewport. It was initially assumed that the viewport possessed an AR coating, which would bring the transmission into the 90% range. Without the coating, it drops to roughly 70%. Assuming no coating, the estimated delivered power was calculated to be 11.7 W. This is consistent with the estimated power given from the Hartmann sensor analysis, thus it is believed that the viewport indeed had no coating.
Quote: |
[Tyler]
Attached below are the initial results of the CIT FROSTI testing analysis.
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Attachment 1: FROSTI_HR_Temperature_Difference-7.png
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586
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Tue Jun 3 11:54:06 2025 |
Cece Ochoa | Update | | CE Cavity Design Update |
Update on the design for the CE Cavity Mirrors |
Attachment 1: CE_Arm_Cavity_.pdf
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394
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Fri Jul 5 14:12:32 2024 |
Liu | Update | Interferometer Simulations | CE BS Mechanical Resonances |
The butterfly and drumhead mechanical modes for the aLIGO BS were calculated in COMSOL. The resonant frequencies for the two acoustic modes are 2.45 kHz and 3.61 kHz, matching the results in reference for instance.
For a quick projection for the resonant frequencies going from aLIGO to CE, the height and width of the BS are increased assuming the mass is increased from 14 kg to 70 kg, while keeping the aspect ratio fixed. The resonant frequencies for the two mechanical modes as a result becomes smaller, to 1.43 kHz and 2.11 kHz respectively, risking getting in the detection band.
Next step is to implement a mechanical ring with high stiffness outside the BS barrel to combat the decrement of the resonant frequencies of the relevant mechanical modes. |
Attachment 1: butterfly.png
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Attachment 2: drumhead.png
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585
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Tue Jun 3 11:50:08 2025 |
Pooyan | Update | CDS | CDS update |
There are three major issues with the lab's CDS system that should be addressed. They are ordered from the highest priority to the lowest.
- CyMAC has stopped serving the fast channels (65k Hz)
The channels are still there, and the data from the slow (16 Hz) channels is served correctly, but the fast data is not served. As a result, diagggui can not retrieve any information at the moment. Probably the issue is the same as the version conflict between daqd and nds2-server. After installing nds2-server on CyMAC and realizing that the conflict can not be resolved, I reverted the changes so that the CyMAC could be compatible with daqd, but there is a chance that there are still version conflicts that block the fast channels. I suspect that we have broken the MSC model when adding the new button. This could explain both the fasr-channels fault and the unexpected crashes.
UPDATE 6/5 Fixes this by rebuilding the models. Note for the future: The c1iop and c1msc models should be rebuilt together, even if no change has been made to c1iop.
- The fast channels were not saved to the frames
Reviewing the frame files showed that the daqd was only saving the 16 Hz data in the .gwf frame files. I had missed this because I only checked the existence and the integrity of the raw frame files, but never retrieved the high-frequency data itself to check it.
- NDS2-server is installed, but does not distribute the data
I managed to install the nds2-server and its satellite programs on the Chimay, and NFS mount the frame files on it. The server successfully chaches the channel names, frame files, and the data, but fails to list the channels for distribution.
Note: CyMAC machine was strangely disconnected from the network, and required manual reboot. I couldn't find any abnormal logs that could explain what happened. |
590
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Tue Jun 10 12:11:14 2025 |
Pooyan | Update | CDS | CDS update |
- The MEDM models issue was fixed. The issue was that building the c1msc model alone was not enough and we had to re-build the c1iop as well, although no changes has been made to the c1iop. Added a note in the wiki on this for future reference.
- For writing the fast channels to the frame files, our CDS system should have a GDS broadcaster. I followed this wiki page to set one, but it breaks the current daqd system. Asked about it earlier today on the CDS Mattermost channel and waiting for a response.
- Maybe I should continue the distributed scheme we have been trying for the nds2-server and let another machine on the network do this.
- Question: daqd has a feature to zero-out the bad data (NaNs), and it is currently on for our system. I don't think that it's a good idea to have this. Should I turn it off?
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592
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Wed Jun 11 16:19:37 2025 |
Pooyan | Update | CDS | CDS update |
- Fast channels recorded to .gwf frame files
- The fast channels are recorded with an extra _DQ in their names. So, in ndscope and diaggui these two channels should be addressed as
- C1:MSC-V0_OUT_DQ
- C1:MSC-V1_OUT_DQ
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Update 6/13: enabled recording of all the ADC voltage channels so that Tyler can use all the data for the noise floor calculation. attached is an example of diagggui with almost 30 hrs of data.
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Attachment 1: Screenshot_20250611_154834.png
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Attachment 2: f3k.pdf
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321
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Tue Feb 13 01:26:30 2024 |
Peter | Update | Interferometer Simulations | CARM Power Simulations |
Cao's simulations of the circulating power and gouy phase through a single arm cavity of the interferometer have been reproduced. Images of the plots can be shown in the pdfs attached. There are approx. 400 lines in this code (scenario_3_carm) that produces these plots. This code also calls on a separate code source file (thermal_models) that defines many of the functions used in this main simulation. The thermal_models file consists of over 1000 lines. More work needs to be done to fully understand and document the scripts. |
Attachment 1: Scenario_3_CARM.pdf
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Attachment 2: Scenario_3_CARM_Gouy.pdf
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199
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Wed Aug 9 17:35:26 2023 |
Shane | Update | CDS | Binary output chassis finished |
Finished the internal wiring for the binary output chassis today, which completes its assembly. Also secured ribbon cables and chassis lid with their respective screws. Note: one of the spade lugs' internal metal piece is a little loose and had to be reinserted after falling out once. Seemed secure after this, and I checked continuity on everything and it was all good. |
Attachment 1: IMG_8685.jpeg
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Attachment 2: IMG_8686.jpeg
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211
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Wed Aug 16 17:17:02 2023 |
Shane, Jon | Update | CDS | Binary input chassis powering correctly |
Binary input chassis passed power-on test, and is lighting up as expected. Binary output chassis also successfully powered on. AA and AI chassis not powering on correctly, need to do some debugging to find the problem. |
Attachment 1: IMG_9253.jpeg
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197
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Tue Aug 8 17:03:22 2023 |
Shane, Jon | Update | CDS | Binary input chassis finished |
Finished assembly of the binary input chassis today, including DC on/off switch and LED installation. external cable assemblies still needed, but internal work done. |
Attachment 1: IMG_8681.jpeg
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537
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Mon Mar 10 21:32:29 2025 |
Nathan | Physics | Electronics | Beam Profiling and PBS Measurements |
Beam wasn't diverging, however maybe was about to diverge when measurements stopped? Will discuss the PBS measurements and how the voltage changed due to the wave plate. |
Attachment 1: Beam_Profiling_2_20_(2).pdf
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Attachment 2: beamprfl.png
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Attachment 3: thumbnail_(6).jfif
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80
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Thu Apr 27 09:48:34 2023 |
Aiden | Summary | General | Batch 12 Bagging |
I took batch 12 out of the oven and put them in a bag and placed the bag inside the clean room in the first large stainless steel container.
I also looked at the small gauge that we felt like needed to be baked and I can confirm that without further cleaning around the inside of the gauge it should not be connected to the main vacuum. I have attached a photo of the inside of the gauge. |
Attachment 1: IMG_4279.jpg
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Attachment 2: IMG_4278.jpg
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510
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Tue Feb 11 08:07:02 2025 |
Luis | Update | VAC | Bake stopped |
[Luis, Ma]
Feb/10/25 4:00pm
Bake was stopped.
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327
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Fri Feb 16 18:37:28 2024 |
Jon | Update | VAC | Bake ended 6:23 pm |
I ended the bake of the UHV system (that began on Monday) at 6:23 pm today by switching OFF both PID controllers. The heaters elements were run at max power (24 V DC / 200 mA per element) during this bake, and I left them powered at the same level.
At the time, the instrument readings were as follows:
- Left high-limit controller: 138 C
- Right high-limit controller: 128 C
- Left PID controller: 100 C
- Right PID controller: 100 C
- Main volume pressure: 8.17e-7 Torr
- RGA volume pressure: 4.63e-7 Torr
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25
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Fri Feb 10 15:15:30 2023 |
Aiden | Update | General | Bagging First Batch |
Aiden Bagged and Tagged the first batch of stainless steel parts shown on the google spread sheet.
1. Removed two parts from the oven.
2. Place them in the ESD bag.
3. Seal bag with Kapton Tape.
4. Create label including part name and number underneath it.
5. Put label onto the side of the bag where it is not sealed with tape.
6. Placed bagged items into clean room on work table.
ps. total bags in first batch = 4 |
324
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Tue Feb 13 12:26:23 2024 |
Tyler | Update | Interferometer Simulations | BS Code Update |
I reproduced Cao's CE beamsplitter code (see below for example plots). I received the current info on the beamsplitter parameters for A+ and A# from GariLynn also. The next steps are to perform a similar power loss analysis on the anticipated A# beamsplitter. |
Attachment 1: thickness1.pdf
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Attachment 2: bs_opd_homloss_h6cm_w2cm.pdf
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396
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Mon Jul 8 10:39:14 2024 |
Xuejun | Update | FLIR | Average Temperature Profile |
After taking data for each of the individual heater elements, I imported them into python and overlayed them to produce an average temperature profile. I rotated the 7 of the elements to align with element 1's profile and averaged them out. By setting the range to 28C - 33C (this gave the best visibility of the heating pattern) it gave the profile attached. |
Attachment 1: Average-Temperature-Profile.pdf
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191
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Thu Aug 3 18:03:42 2023 |
Shane, Jon | Update | CDS | Anti-Aliasing chassis complete |
We finished installing the internal power supply cables in the anti-aliasing chassis today, which concludes its assembly. Work on AI, BI, BO chassis still underway. |
Attachment 1: IMG_8544.jpeg
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154
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Thu Jul 13 15:31:21 2023 |
Jon | Update | General | Ant traps placed around lab |
In response to reports that ants have been observed in the lab, I placed five ant bait traps around the room today. Each is sitting on the floor on top of a piece of aluminum foil, in areas unlikely to be inadvertently stepped on. They contain liquid which will spill out if picked up, so please take care not to disturb them. |
155
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Thu Jul 13 16:59:03 2023 |
Jon | Update | General | Ant traps placed around lab |
Update: After seeing the strong response to the first set, I redistributed them to the hottest spots and added one more trap.
Quote: |
In response to reports that ants have been observed in the lab, I placed five ant bait traps around the room today. Each is sitting on the floor on top of a piece of aluminum foil, in areas unlikely to be inadvertently stepped on. They contain liquid which will spill out if picked up, so please take care not to disturb them.
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598
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Tue Jun 24 13:47:58 2025 |
Liu | Update | Interferometer Simulations | Alternative FROSTI A# optimization approach |
Alternative FROSTI A# optimization approach |
Attachment 1: Update.pdf
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63
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Tue Apr 4 16:43:53 2023 |
Jon | Update | VLC Electronics | Additional Thorlabs PDA10A2 |
I ordered a second PDA10A2 and mounting post + spacer (which puts the aperture at the VLC's standard 3" beam height). These arrived today and I delivered them to the lab. They are sitting on the VLC table near the laser. |
Attachment 1: PDA10A2.png
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14
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Wed Dec 14 18:34:33 2022 |
Jon | Configuration | Electronics | Adapter for 532 nm laser power supply |
I installed an EU-to-US plug adapter for the 532nm laser's 9V power supply. I then re-measured the laser's power with the correct supply voltage (previously we had been using a 6V supply). At 9V, the max power is 0.83 W, so the laser is confirmed to be Class 2 as labeled. |
Attachment 1: laser_power.png
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142
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Mon Jul 3 16:26:21 2023 |
Cao | Infrastructure | DAQ | Access and control Red Pitaya remotely and run it on local machine |
[Cao]
To access and control the Red Pitaya using Python locally on a machine within the local network, one should follow these steps:
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Start the SCPI server. This is achieved by first log onto the Red Piatay page
rp-xxxxxx.local/
- Go to Development >> SCPI server and turn the server on. (Note : The server is currently running)
- Communication with Red Piataya is done through PyVista, install PyVista with:
sudo pip3 install pyvisa pyvisa-py
This has been installed on Chimay. Ensure that you have pip3 install, if not, you can install it using:
sudo apt-install python3 pip
- To start talking to the RedPitaya, ensure you have the scipt
redpitaya_scpi.py in your local folder. This is the standard class that you will import to your code to establish connection with the Red Pitaya. This code can be found in directory ~/RedPiatya or this link
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399
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Tue Jul 9 18:19:50 2024 |
Shane | Update | CDS | ADC-DAC loopback testing and IOLAN installation |
[Shane, Jon]
Finished ADC-DAC loopback testing today (see attached xlsx file or access directly here). All looks well with the first 8 channels, with the gain hovering just under 2. Also edited c1msc model in simulink to add channels 7-15 (the last 8 channels), and changed the rate back to 64K. See image 1 for the updated c1msc model. The last 8 channels are also looking good and show no problems, with slightly more scattering for the gain, but all values very close to 2.
We also installed the new eight-channel Perle IOLAN SDS8 terminal server today. Image attached.
NOTE: When we were installing it, we noticed an energized wire dangling from the 24V power supply. Has since been fixed and put back into place. |
Attachment 1: iolanServerTerminal.jpeg
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Attachment 2: ADC-DAC_Loopback_Testing.xlsx
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Attachment 3: updatedc1msc.jpeg
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410
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Tue Jul 16 18:43:07 2024 |
Shane | Update | CDS | ADC-DAC loopback testing and IOLAN installation |
UPDATE:
Follow up ADC-DAC loopback testing now complete, matching all the ADC channels to a single DAC channel, and then matching all the DAC channels to a single ADC channel (see attached xlsx file or access directly here). Also note c1msc model file has been updated to include the second set of 16 ADC channels. The newly added channels also have their own filter modules, but those are not needed for anything other than the loop-back testing and can now be deleted if we don't want to keep them.
Quote: |
[Shane, Jon]
Finished ADC-DAC loopback testing today (see attached xlsx file or access directly here). All looks well with the first 8 channels, with the gain hovering just under 2. Also edited c1msc model in simulink to add channels 7-15 (the last 8 channels), and changed the rate back to 64K. See image 1 for the updated c1msc model. The last 8 channels are also looking good and show no problems, with slightly more scattering for the gain, but all values very close to 2.
We also installed the new eight-channel Perle IOLAN SDS8 terminal server today. Image attached.
NOTE: When we were installing it, we noticed an energized wire dangling from the 24V power supply. Has since been fixed and put back into place. |
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Attachment 1: Follow-up_ADC-DAC_Loopback_Testing.xlsx
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285
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Mon Dec 4 21:27:53 2023 |
Shane | Update | CDS | ADC-DAC loopback test results |
Here are the test results from today's ADC-DAC loopback tests. Channels 14 and 15 were the only ones behaving abnormally. Not sure what the issue is, but needs further debugging. The DAC output was as expected for both of them, but the corresponding ADC inputs were the same regardless of what offset was used (hovering around values of -4 and -5). NOTE: all measurements listed in the attached table are 'averages' in the sense that the ADC inputs and DAC outputs hovered around the listed values, changing by +1 or -1. |
Attachment 1: adc-dac_loopback_testing_results.pdf
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176
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Thu Jul 27 14:46:55 2023 |
Shane, Jon | Update | Electronics | AA chassis DC on/off switch assembled |
Made the first DC on/off switch assembly today and installed in anti-aliasing chassis. Second switch assembly to be completed later. |
247
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Fri Oct 27 15:28:30 2023 |
Shane | Update | CDS | AA and AI chassis for CyMAC powered on and functional |
CyMAC updates: Switched out the faulty power regulator boards in the Anti-Aliasing and Anti-Imaging chassis. Both chassis are now powering up correctly with lights on and the correct voltages in/out of the power regulator board. Images attached. All chassis for the CyMAC now functional, so next step is mounting everything in the rack. |
Attachment 1: AI_chassis_lights_on.jpeg
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Attachment 2: AA_chassis_lights_on.jpeg
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577
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Tue May 13 12:41:06 2025 |
Tyler | Update | TCS | A# Profiles Update |
Slides on the A# ITM FROSTI profile modeling efforts can be found here. |
602
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Tue Jul 1 12:39:42 2025 |
Tyler | Update | TCS | A# FROSTI Profile Optimization Update |
[Tyler, Liu]
Slides |
632
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Tue Aug 19 12:33:59 2025 |
Pooyan | Update | TCS | A# BS Update |
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Attachment 1: A#_beamsplitter_thermal_lensing.pdf
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209
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Tue Aug 15 16:10:06 2023 |
Celeste | Update | TCS | 8/15/2023 Simulation Progress |
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Attachment 1: Simulation_Progress__1_32nd_Model_(2).pdf
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204
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Fri Aug 11 10:57:20 2023 |
Celeste | Update | TCS | 8/11/23 Simulation Progress |
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Attachment 1: Simulation_Progress__1_32nd_Model_(1).pdf
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200
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Thu Aug 10 14:13:38 2023 |
Celeste | Update | TCS | 8/10/23, Simulation Graphical Progress |
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Attachment 1: Simulation_Progress__8_10_23.pdf
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88
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Mon May 1 18:56:57 2023 |
Peter | Update | VLC Electronics | 532nm Intensity Measurement |
I've configured the two PDA's to the Red Pitaya. I put a 50 ohm resistor connector to each red pitaya input port. This was because the oscilloscope showed that the voltage reading from the P polarization PDA was almost at 1V, which was the limit of the red pitaya. Once both S and P polarization PDA's were connected, I opened the red pitaya's oscilloscope. A screenshot of the voltage readings is shared below. Channel 1 (Yellow) is for S polarization. Channel 2 (Green) is for P polarization. It would seem that there is a significant amount of polarization in the P direction as opposed to the S direction.
I then tried running the template time series measurement within the python notebook from channel 1 only. The python notebook graph is shown below. I have not figured out what are the units of time on the x axis, and I have not figured out how to change the amount of time that the red pitaya takes data. A plot of the time series measurement is shown below. |
Attachment 1: graphs.jpg
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Attachment 2: Time_Series_Trial_1.png
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89
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Tue May 2 15:55:33 2023 |
Peter | Update | VLC Electronics | 532nm Intensity Measurement |
I changed the 1/2 wave plate from the lens mount to the rotational optic mount. This allowed me to rotate the 1/2 wave plate, which changed the respective polarization power transmitting through S and P polarization. Initially, more power was coupled into the P polarization. Now, with the 1/2 plate rotated, both channels are experiencing the same voltage reading. Before feeding the PDA signals into the red pitaya, a 50 ohm terminator had to be placed at the SMA connection port so that the input power into the red pitaya did not exceed 1V. With this configuration, both channels experience about 0.35mV. (See attached)
I then opened the Jupyter notebook, and ran a demo time series measurement from the red pitaya. This time, I was able to get a plot featuring both channels (green is P polarization. Blue is S polarization). The plots are consistent with what is shown in the red pitaya oscilloscope. However, the time collection (I'm assuming) only runs for about 0.018s. I will have to write some of my own code to loop over this measurement, and collect more data. |
Attachment 1: IMG-0221.jpg
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Attachment 2: IMG-0222.jpg
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Attachment 3: graphs(1).jpg
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Attachment 4: Time_Series_Trial_2.png
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92
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Thu May 4 14:01:10 2023 |
Peter | Update | VLC Electronics | 532nm Intensity Measurement |
I adjusted the rotational mount of the wave plate to see if the power can be 100% coupled into either S or P polarization. The images shown below of the oscilloscope indicate that this is not possible. The minimum transmitted power we can obtain in either S or P polarization is 75mV. The maximum voltage we obtain in either S or P polarization is ~ 740mV. This means that at a maximum, we can obtain ~ 90% polarization in either direction, indicating that our laser has a slightly elliptical polarization. |
Attachment 1: graphs(3).jpg
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Attachment 2: graphs(2).jpg
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Tue May 16 11:56:33 2023 |
Peter | Update | VLC Electronics | 532nm Intensity Measurement |
With the configuration the exact same as before, I used the Jupyter notebook in the red pitaya's development package to collect data from both input channels. Last week, I was able to take data, yet only for a very short period of time, and I did not know how to change it. I went online to the red pitaya's user manual to figure out how to change the sampling period for longer. The link to the page is here: https://redpitaya.readthedocs.io/en/latest/appsFeatures/examples/acqRF-samp-and-dec.html#s-rate-and-dec Though I now know how to change the period of time for which data is taken, the maximum amount of time is still only about 8 seconds. So with help from Cao, we looped over the data taking samples, and got a mean value for each iteration. We then put all those mean values in an array, and plotted it. Below, we see a plot of both the S and P polarizations, and a sum of both of them. As seen in the graph, I have set the time to be able to take data for almost 2 minutes. There is some slight drift in the respective intensities. The next steps I believe are to convert the units into watts, and take data for longer periods of time. |
Attachment 1: Time_Series_Trial_3.png
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101
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Thu May 18 14:07:08 2023 |
Peter | Update | VLC Update | 532nm Intensity Measurement |
I figured out a method in which to capture power measurements including the initial seconds in which the beam is first turned on. I first clear and restart the kernel of the python notebook. Then I run the command to connect the red pitaya oscilloscope package to the input data being taken in both channels. To my understanding, this allows for data acquisition as the code compiles. I then started looping the 1.074s trigger bunches, and then roughly 2 seconds after I ran that command, I went and turned on the laser. The first plot shown is a 2 minute practice trial of me trying this technique to make sure that the python package was correctly registering the input of the red pitaya. It is clear that initially the laser is off, and then as I turned it on, the voltage in each channel spikes, which is compelling evidence that the code is working. I then set the data collection to be 7518 seconds (7000 loops), which is about 2 hours and 5 minutes. I repeated the same technique as for the first plot, only changing the amount of time I collected data. The second plot shown here is the voltage being read in each channel as a function of time. As we can see, over a period of hours, the intensity drifts quite dramatically for the first several minutes, and then begins to stabilize slightly. However, there are still some strong sudden fluctuations in each channel. |
Attachment 1: Time_Series_Trial_4.png
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Attachment 2: Time_Series_Trial_5_2hrs.png
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36
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Tue Feb 28 19:31:05 2023 |
Peter | Update | VLC Electronics | 532 M2 Measurements |
Took M2 measurements today. Configuration: Lens 1 (f = 50mm) at 0mm. Lens 2 (f = 150mm) at 200mm, camera at 350mm. The laser beam was being moved in -z direction on track (so further away from the first lens). Quick data shown in the sheets plot. Not a real fit. I was trying to see where the beam waist was if there even was one. Seems that it is much further than we have room for on the track. Will need to come back and take more data.
I suggest maybe Dr. Richardson or Cao come and see the configuration in person and how the beam diverges for themselves on the detector card. Maybe they can offer pointers to make this go smoother. |
Attachment 1: X_width_and_Y_width.png
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37
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Tue Feb 28 19:33:51 2023 |
Peter | Update | | 532 M2 Measurements |
Y axis of plot in units of micrometers. X axis in units of millimeters. |
48
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Thu Mar 9 12:03:59 2023 |
Peter | Update | VLC Electronics | 532 M2 Measurements |
Took more M2 Data today. Picture of the optical set up is shown below. lens1 f = 100mm, lens2 f = 50mm, lens3 f = 150mm. There was a nice converging/diverging beam profile, and the beam waist was able to be read by the camera. I took as much data as I could before clipping loss. The M2 value is quite high. |
Attachment 1: OmegaY_M2_Fit_3.png
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Attachment 2: OmegaX_M2_Fit_3.png
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Attachment 3: optical_setup.jpg
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50
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Fri Mar 10 12:08:09 2023 |
Peter | Update | VLC Electronics | 532 M2 Measurements |
Took more M2 laser data today. The configuration is the same as before except now the beam camera is the only component moving. Pictures can be seen below. The beam shape in x and y is very consistent with low error. However, the M2 value is still a bit high. |
Attachment 1: OmegaX_M2_Fit_4.png
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Attachment 2: OmegaY_M2_Fit_4.png
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Tue Apr 4 09:39:58 2023 |
Peter | Update | VLC Electronics | 532 M2 Measurements |
Final M squared measurements were taken Wednesday, 3/29/23 by Peter and Ryan Hinosawa. 5 separate sets of data were taken, and upon discussion, we declared the plots shown below in attachment 1 and 2 as the final plots of our M squared measurements.
The optical design of the M squared measurement process is given in attachment 3. The laser and three lenses shown below are mounted on the optical table. The track is placed behind the third lens, and the camera is moved along the track to take successive measurements of the beam's width. This will allow us to see a change in the beam's width over its propagation direction.
The raw data is given in attachment 4 as a Beam_Data_8_3lens.txt file. This is eventually what gets used to generate the plots shown below.
The code to run the analysis on these measurements (as well as analysis on the Gaussian intensity profile fitting) can be found:
git@git.ligo.org:uc_riverside/visible-light-cavity.git |
Attachment 1: OmegaY_M2_Fit_8.pdf
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Attachment 2: OmegaX_M2_Fit_8.pdf
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Attachment 3: M2_Measurements_Set_Up.svg
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Attachment 4: Beam_Data_8_3lens.txt
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z-z0 x_width y_width x_error y_error
-50 267 304 30 30
-40 227 261 30 30
-30 192 223 30 30
-20 167 194 30 30
-10 153 169 50 50
0 149 154 50 50
10 166 152 50 50
20 198 169 50 50
30 233 195 50 50
... 17 more lines ...
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Fri Sep 29 11:53:54 2023 |
Shane | Update | Cleanroom | 5 zone particle count measurement in cleanroom |
Today's 5 zone measurement of cleanroom particulate concentration is attached |
Attachment 1: 23.png
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Attachment 2: 23.png
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270
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Fri Nov 17 14:06:01 2023 |
Shane | Update | Cleanroom | 5 zone particle count |
Here's today's 5 zone particle count measurement for the cleanroom. Zone 5 (closest to back wall by fire cabinet) is still above the limit for the larger size ranges; everything else is in good shape and roughly 10 times under the limit. Not sure why zone 5 is still so dirty (maybe some of the electronics being stored in bags/bins on the upper shelf of the desk aren't clean?) but will focus cleaning efforts on this zone next time. |
Attachment 1: 23.png
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260
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Thu Nov 9 19:06:46 2023 |
shane | Update | Cleanroom | 5 zone cleanroom measurement |
Here's today's five zone measurement, taken ~5 hours after the cleaning. Zone 5 (closest to fire cabinet and back wall) is a bit over the limit in all size ranges (about 1500 particles in 1.0u size range over), and zone 2 is slightly over the limit in the 1.0u range, but everything else is under the requirement. |
Attachment 1: 23.jpeg
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619
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Tue Jul 29 12:30:00 2025 |
Christina | Update | TCS | 260 hour ADC update |
[Ma, Christina, Tyler]
ADC CyMAC 260 hr, 8192Hz sampling rate channels V3 and Vref6 |
Attachment 1: CSD_06_28_25_270hr.png
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