Hi all,
first of all, thanks brianpe to your suggestions, nice website and instructions! One rarely sees those with such high quality.
Over the last few weeks, although I didn't have much time to work on the laser, I did have some correspondence with some authors of DPSS TiSa papers who gave me some valuable tips. First of all, I have abandoned the X-fold resonator, too many variables and doesn't fit well on my optics table (too short arm lengths). I did try the alignment technique mentioned in Steve's manual, I actually saw all the mentioned spots, but no luck. I also switched from a 5% OC to a 2% OC. Now that I write this, I didn't actually try the X-fold setup with the 2% OC - I'll do that tomorrow. My crystal is now water cooled, stays below 20°C.
These are the tips from the researchers - maybe they'll be useful to someone else:
Pretty much all of them mentioned that my pump mode radius may be too large - I think this is the root of the trouble I am having right now. I measured them using a razorblade and a translation stage (google "knife edge method", my cut-off is ~11%, not 1/e²) and my green beam is 35x40um and the blue beam is 30x70um. Note that in the crystal one dimension is expanded by 1.7, the refraction index of TiSa. Usual values in the literature tend to be around 20um, but especially the green diode is actually similar in power and size of some published articles so it should generally work..
Another tip (for the folded resonator, type 2 in the original post) was to use the fluorescence spots to align the two curved mirrors and then an amplified photodiode to align the flat OC. I did all that, aligned the spots and tuned the OC to the maximum value on my photodiode, but sadly no lasing.
I also received the tip of removing one arm by folding the beam into the curved mirror (essentially replace X-fold with V-fold resonator), which is what I already did so I know this should work in theory.
Polarization does actually matter, as Steve said. Ti:Sa absorbs light much more (factor depends on doping, but can be around 2x) in one polarization than in the other. Luckily, both my 520nm diode and one 465nm are correctly oriented so this is not an issue. The difference in color between the 465nm diodes is astounding - in the correct orientation, the crystal is a lot pinker as the more blue light is absorbed and turned into fluorescence.
One of the researchers said that 200mm arm length may be too short although the cavity it self is stable. longer arm length - tighter mode radius between the curved mirrors. Unfortunately my breadboard is not very big.. So I used a HR mirror to extend the arm, now it should be around 550mm which is in the realm of what the literature reports (although 200mm can be found as well).
The folding angle is important and must be calculated correctly - I checked this at least 5 times, it is correct.
One of the resarchers also emphasized that TiSa is very sensitive to losses, I think Steve hinted at this already. I needs to be cooled, used at brewsters angle and with low OCs (1-3%). I have 2% so that should be alright.
I have read consistently that powers as low as 1-2 W should be enough to lase (some researchers also told me this in their emails). Thats encouraging, but also quite frustrating since I feel that I am doing everything right but no lasing.
Here are two videos of the setups and me trying to align the resonator by overlapping the fluorescence spots.
Vid1 Here you see the setup. I taped some orange plexi infront of my phone camera, filters out all of the green pump light.
Vid2 Changed the mirror distances a bit, so the spots look different. Interestingly, here you can see a very faint third spot which can be moved by moving the OC. Aligning all three spots (in my mind) guarantees perfect resonator alignment, but no lasing.
To anyone with experience in this field: Are the spots supposed to be equally big like in Vid1 or can they be differently sized like in Vid2?
My alignment process is as follows, btw: I remove the OC and use a 808nm beam (same wavelength as the TiSa output!) to align the curved mirrors by inserting a pinhole at the OCs location and moving the curved mirrors until the reflected spot goes through the pinhole. Then I insert the OC and move it to reflect the 808nm directly into the 808 source.
For fine adjustment, I use the fluorescent spots like shown in the vids.
After probably 100 hrs of alignment, I can get all spots aligned from scratch in about 20 minutes, I am very certain that alignment is not the issue. So, after ruling out this, polarization, wrong outcoupling, crystal cooling, resonator stability (I am using reZonator 2.0), folding angle and too low power, only four issues are possible:
1. Pump radius too big. Most likely. Although I am using the exact same green diode as one paper, maybe it is damaged, idk. I have also tried a galileam beam expander to get smaller focus radii, but it introduced a lot of spherical aberrations.. Although the core spot is indeed smaller.
2. Haven't found the perfect position of the mirrors spacings yet, even after so much time. In my mind unlikely, but definitely possible, I'll keep trying.
3. The crystal or mirrors are defect/wrong specs. Steve mentioned this and I ruled it out, but at least the eBay stuff might not be what it says it should be, although both sellers are reputable. Thorlabs and Optogama I trust. I'll have to go to my uni's optics lab to check all the mirrors and the crystal.
4. Dust flying in the air introduces high losses. My basement is not extremely dusty (still cover all the optics when not in use) but maybe clean room conditions are mandatory? Idk.
If nothing works, I'll look for smaller power diodes with better M² (which is usually the way in the literature) and ask my optics faculty to measure the optics.. But since I'll be going to the US for 6 months next week, this - very much to my frustration - will have to wait.
Sorry for the long post - As Steve said, this project is very complicated. As always thoughts on my notes are appreciated!
~Nik
PS: I have attached a screenshot of the ReZonator simulation, this is the very latest iteration of the resonator.