Kinds of lasers

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So you want laser guns, and you also want to know how they work. One place to start is by looking at how people have already got lasers to work. There are a lot of very clever people in this world, and they’ve tried a lot of inventive ways to get lasers to do their thing. I’ll cover some of the more well known and promising high powered laser technologies here. [1] Note that if you have some futuristic society where laser pistols are effective sidearms, they will have developed some new technology not on this list. We’ve got some pretty good lasers these days - but not that good.

Carbon dioxide lasers

CO2 lasers were one of the first practical high power lasers. As you might have guessed from the name, they use carbon dioxide gas as their laser medium, typically excited into lasing by an electric discharge. [2] The carbon dioxide in one of these lasers might not cause much global warming, but it sure can cause a lot of local warming! They are useful in industry because they are relatively cheap and efficient, commonly turning upwards of 20% of the supplied electricity into laser light. However, they emit beams in the long-wave infrared. This is problematic for using them as any kind of weapon, because those long wavelengths don’t focus very well at typical combat ranges. The long wavelength light is also easily absorbed by plasma, and at high intensity it is all too easy to get a runaway cascade ionization going that stops your beam. So while they might be used to weld fighter jets together, CO2 lasers are not the best choice for burning fighter jets out of the skies.

Chemical lasers

Back in the 20th century, people were trying to figure out how to make really high powered lasers. Rocket engines are really high powered, right? So how about taking a rocket engine, burn some special chemicals as fuel in the rocket, run an optical cavity across the nozzle, and use that energized burned fuel shooting out for the laser? And you know what? It worked. [3] You get a nightmare of tubes and plumbing like any rocket engine, tanks of highly volatile toxic corrosive and flammable chemicals, lots of noise, flaming jets of toxic corrosive exhaust, and megawatt beams of poorly focused and poorly focusable laser death. Some of these lasers were used as proving grounds to advance important aspects of laser technology or exploring its applications [4] [5][6] [7] , but no one wanted to deal with the chemicals. So they were abandoned as soon as possible in favor of electric lasers.

The two most promising chemical lasers from a “blow all the bad guys up” perspective were the deuterium fluoride (DF) laser, which emitted light in the mid-wave infrared part of the spectrum at 3.8 μm in the atmospheric transparency window, and the chemical oxygen-iodine laser (COIL), which produced near infrared light at 1.315 μm wavelength.

Diode lasers

Semiconductors do this weird thing where they conduct electricity both with electrons and with the lack of electrons. A particle of a lack-of-electron is called a hole, and you can think of it as a missing molecular bond if you wish, and the missing bond can move around the crystal by borrowing the electron of a neighboring chemical bond - moving the hole to that chemical bond that was borrowed from and repairing the previously broken bond [8] . This isn’t the place for a lecture in solid state physics, but the main idea is that in a diode you mix an electron current with a hole current and when an electron falls into a hole, it takes the place of that missing molecular bond and can emit a particle of light in the process. If you do this inside an optical cavity, you can get lasing.

Now during the 20th century we got very good at working with semiconductors. So perhaps it is not surprising that we can make very nice diode lasers. They’re tiny little things, perhaps the size of a grain of rice, and sometimes packed together in parallel into large bricks. By adjusting what we dope the semiconductor with and how we layer and arrange the semiconductor layers, we can get beam colors ranging from ultraviolet-C to far infrared. The efficiency can be crazy high - 60% electricity to light or better. They are cheap and robust and found all over the place in modern consumer electronics. [9] [10]

For making laser death beams, however, they have one annoying limit. You can get high powers out of them, but when you do so they start to lase on all kinds of different modes and their beam quality goes to hell. If you can’t focus them better than a flashlight, you’re not going to be using them to burn your enemies out of the sky.

The usual way to get around this is to use cheap, highly efficient diode lasers to pump other kinds of lasers that need light to get their laser action going. That way we can use a fiber laser coil, for example, to convert poorly focusable diode laser light into extremely focusable light from the fiber laser.

Solid state lasers

The first laser ever made was a solid state laser. It was made with a ruby crystal. While it might seem neat to use lasers with gems as the laser generator, there were better options. Today, solid state lasers are made with slabs or rods of garnet crystal called yttrium-aluminum-garnet doped with the rare earth element neodymium, abbreviated Nd:YAG. Early Nd:YAG lasers were pumped with xenon flash lamps, and had abysmal efficiency (around 1% or less). Then mankind invented semiconductor technology, made laser diodes, and used the laser diodes to pump the garnet crystals instead. Now the efficiency got to higher than 30%. The Nd:YAG turned out to be excellent at taking badly focused diode laser light and efficiently turning it into near diffraction limited focused laser light at 1.064 μm wavelength in the near infrared. You could even shoot the beam through a nonlinear optical crystal and upconvert two 1.064 μm photons into a single 0.532 μm photon, and get green light at 80% conversion efficiency. You can even get higher harmonic conversion to 0.355 μm, 0.266 μm, and 0.213 μm wavelengths in the near ultraviolet.

Meanwhile, a different kind of solid state laser was gaining popularity. If you dope a sapphire crystal with titanium, you can get it to lase on a very wide band of colors spanning the near infrared and even a bit into the red part of the spectrum. This ends up being useful because a single frequency technically only defines an infinite duration wave. In order to make a waveform that starts, operates for a while, and then stops you need to broaden that spectrum a bit, mixing in waves with slightly different frequencies that add up together at times when the beam is on but cancel out when the beam is off. And the shorter the pulse of the beam, the wider the range of frequencies need to be in that pulse to get it short enough. Normally you can ignore this effect, but if you want to get very short pulses - picoseconds or femtoseconds long - the spread in frequency starts to be important. And if your laser can’t amplify those frequencies you can’t get such short pulses. So titanium sapphire lasers were used to make these incredibly short laser pulses. By compressing what would normally be a fairly moderate amount of energy into crazy-short time spans, titanium sapphire lasers could reach powers and intensities that were off the charts. They don’t give pulses that have as much power as a Nd:YAG laser, and their average power is overall lower, but for instantaneous power during their pulse they can’t be beat.

Soon, Nd:YAG lasers became the workhorses for just about any application that needed a high powered laser; and Ti-saphhire lasers were in common use for producing ultra-short, extreme power pulses. They became common in medicine, machining, science, and all sorts of other fields. Many were investigated for military laser weapons. They could direct tens of kilowatts of infrared death onto incoming missiles and mortar shells and other flying things. The main annoyance was that with high power came heat, and heat warpend and expanded the crystals, which degraded the quality of the beam. Various clever designs were used to cool the crystals. But eventually they were replaced by …

Credit

Author: Luke Campbell

References