Oh, This is not so hard. I work on three phase ion lasers, with 35-60 amp plasma currents to generate the lasing.
The current is regulated by 18 to 36 NPN transistors (depending on model) ran common emitter in parallel. There are also some smaller plasma tubes that need 9-10 amps and run off 110 AC. These are regulated by a high side buck switcher using a few big mosfets as a constant current source. I'll admit that a 1600 watt 160 VDC constant current buck is not that small a PSU.
The small ones use a 600V or 1200V 60 amp blocking diode, an inductor wound on a ferrite bar, and a metal can mica return capacitor (600 WVDC, 0.1 uF) to keep the ringing wave from the HV transformer out of the PSU. The cap provides a LF return path for the igniter, whether the tube fires or not. These use series injection triggering, and the secondary of the igniter carries the full plasma current. The small ones have a boost cap ~1 uF charged to 600-800 volts and coupled using a blocking diode to have a little extra voltage to ensure the plasma forms a "cathode spot" on the tube cathode that can emit electrons. Welding is also dependent on forming a "cathode spot" of intense electrons to start and sustain the plasma.
The igniter is high side series injection triggering up to 36 KV. The trick is to use a decaying, ringing wave, superimposed on the DC. Typically 100 KHz to 500 KHz. This way a simple LC low pass filter and a metal can, mica "return capacitor" can be used to keep the HVDC out of the transistors and filter caps.
For small systems, the igniter is a big toroid with 30 turns of # 8 on the secondary and a one to two turn primary. 400 VDC is dumped into the primary via a industrial grade SCR from a 1-10 uF cap, depending on model. A reverse diode across the SCR protects it from frying. A small ceramic cap across the secondary resonates it.
On the big systems brand "A" uses a series injection transformer designed for xenon flashlamps and capable of carrying 60 Amps thru the secondary. We call the return capacitors "bathtub" caps, because they look like a little metal bathtub, with a lid soldered on. Brand A has a large inductor in the hot side, the bathtub cap to ground, and then the igniter coil. The plasma tube serves as a spark gap if it does not light the plasma.
Brand B does things a little differently, They have a ferrite rod inductor that has about 15 turns of # 10 copper magnet wire to keep the HF out of the DC from the PSU on the hot side. Right after that they have a spark gap (air gap) that couples the igniter pulse from a classical flashlamp style HV transformer into the tube anode. The bathtub cap is on the high or PSU side of the inductor for brand "B" as a secondary means of protecting the PSU.
Moral of the story, igniter pulses need a "AC" return to ground independent of the load. Usually a small return cap sized to conducts RF but almost nothing else is across the load to close a loop around the ignite pulse. key word here is LOOP, you do not want to shunt the whole HV ringing wave to ground.
Classical Arc and Tig Welders with HF ignition have a sort of tesla coil and a LC filter network and spark gaps to keep the igniter waveform out of the rectifier diodes and control system.
Wima makes or made the mica caps used in all brands of the lasers. While they are only rated 600 WVDC, they comfortably shunt 20-30 KV pulses to ground, provided there is a plasma tube there to break down.
A 1" arc length xenon strobe tube from a disposable camera breaks down at ~1200 VDC in my bench tests. I've used them as spark gaps for that reason, and you can also get gas discharge overvoltage protectors for a few dollars to protect your caps from rogue pulses.
Make sure your igniter has a ringing wave so you can filter it out.
Have fun designing the filter inductors, however keep in mind the ignite pulse should be 5-10 cycles of ringing, decaying wave, so your not too worried about the inductors saturating if the plasma does fire and start welding.
This should take a load off your mind about having a large inductor messing up your double pulse waveforms.
If your weld plasma fires, you can pretty much bet that will shunt the ignite pulse. It is what happens when it doesn't fire, that concerns you. In that case the ignite spike wants to break down the insulation in your storage caps.
I wish I could show you the inside of one of the PSUs I work on. For a 20,000$ laser, they are quite simple, just banks of water cooled NPNs controlled by a few op-amps, and the newer ones are 7-10 kW buck switchers..
We have a Sunstone upstairs, but there is no way that department is going to let me pop the cover for pictures.
I've used it, I see no evidence of a huge HV ignite spark if we don't get a weld. They may be doing things differently, such as flowing a "Simmer" current right before they pull back the electrode. The simmer current would be just enough to start a pilot arc between the tungsten point and the metal to be welded. Quite honestly, they have some circuitry to prevent it firing if conditions are not perfect. We often get movement of the rod but no weld or even a spark when holding the probe freehand.
It will not fire unless the tungsten tip is FIRMLY in contact with the object to be welded. I think they measure the resistance of the contact before firing. As I said, if things are not perfect, it will pull back the tip when you hit the pedal, but there will be no attempt at a weld.
I'd also think Sunstone would warn of us of a potential "sting" if they used a free running start pulse. There is no such warning.
Steve
PS some reading:
http://laser-caltech.web.cern.ch/laser-caltech/report/Flash%20lamp%20Eg&G.pdfhttp://www.repairfaq.org/sam/532hsch.gif (T1 is the igniter toroid, note the blocking diode)
http://www.excelitas.com/downloads/dts_triggertransformers.pdfhttp://pulsearcwelder.blogspot.com/ (mentions lift start and HV pulse start)