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Why lasers work › Part 3 of 3

How CO₂, Fiber, Diode and UV Lasers Actually Generate Light

By Brandon Cullum • Last updated Aug 5, 2026

So I published the review. Diodes can't match CO₂ on wood. Showed my test results. Explained the physics.

And oh man, the comments.

"Just tune the wavelength to 10.6 microns."
"There's gotta be a setting."
"You obviously don't know how to use it."

Look. I get it. I wanted there to be a setting. I spent $600 on diode lasers trying to make them work. But wavelength isn't like speed or power. You can't just "adjust" it.

Wavelength is locked by physics. Not software.

This page is the receipt for that sentence. Every wavelength in this guide has been treated as a given: a CO₂ laser puts out 10,600 nm, a diode 450 nm, a fiber 1,064 nm. Each laser type stores energy in a different kind of jump, and the size of that jump is the wavelength. Change the wavelength and you have changed the gas, the crystal or the dopant.

If the marketing had been honest, "20W at 450nm" against "50W at 10,600nm", people could've googled "what wavelength cuts wood" before buying. But "watts" sounds simple. And simple sells.

If you have not read the earlier parts, start with what the four laser types do in a shop and why materials absorb some wavelengths and not others.

How each laser type makes its light

Close-up of a fiber laser mid-fire on the metal head of a claw hammer, a burst of sparks and a red aiming dot at the point where the beam lands.
A fiber laser engraving a hammer head, sparks and all. This is the light this section explains, at the moment it meets metal.

What all four have in common

Before the differences, the two things every laser on the list does identically. Explaining them once means the four sections below can be about what actually makes each machine different.

Population inversion. In any normal gas or crystal, nearly everything sits in its ground state and maybe one in a million is excited. A laser flips that: you pump energy in hard enough that more of the medium is excited than is not. It matters because a photon travelling through has two possible fates. Hit something in the ground state and it gets absorbed and disappears. Hit something excited and it triggers that thing to drop, surviving and creating a second identical photon alongside it. With mostly ground-state material, photons vanish faster than they multiply and the light dies. With mostly excited material, light grows exponentially. One photon becomes two, two become four, four become eight. That is stimulated emission, the SE in laser, and it is the entire difference between a light bulb and a beam.

The cavity. Every one of these has mirrors at both ends of the gain medium. One reflects everything, the other lets a fraction through. Photons bounce back and forth hundreds of times, triggering more emission on each pass. Anything travelling at an angle hits the wall and is lost, so only photons running perfectly parallel to the axis survive the round trip. The partial mirror lets those out, and that is your beam: billions of identical photons all going exactly the same direction. What differs between the four is the gain medium and the shape of the cavity around it, and nothing else.

Close-up inside a laser machine of a round mirror held in a black bracket with adjustment screws, part of the beam path.
One of the mirrors on its adjustment mount inside a CO₂ machine. Mirrors like this are why only the photons running straight down the axis survive to become the beam.
A long glass CO₂ laser tube with coolant fittings and wiring, lying in the rear compartment of a laser cutter.
The CO₂ tube in the back compartment of a machine, which is the sealed glass the gas mix sits in. The electrode at each end is what puts 20,000 volts across it.

Pick a laser type to see what makes it different:

The interesting part: nitrogen does the work

A CO₂ tube is not filled with CO₂. It is filled with CO₂, nitrogen and helium, and the nitrogen is there because it is a better middleman than electrons are.

N₂ has a molecular weight of 28 against CO₂'s 44, so free electrons get it vibrating far more easily. Lighter cart, easier push. And N₂'s vibrational energy level happens to sit almost exactly on CO₂'s first excited state, so when an excited N₂ collides with a CO₂ molecule the vibration transfers cleanly, the way one tuning fork sets off another tuned to the same note.

Electrons to N₂ to CO₂ is measurably more efficient than electrons straight to CO₂. That indirect route is why the gas mix is what it is.

Getting there from a plug socket

The tube is sealed glass with a metal electrode at each end carrying 20,000+ volts. Switch it on and that voltage rips electrons off the gas molecules, creating a glowing plasma of free electrons moving fast enough to act like tiny billiard balls.

CO₂ can take that hit because it is lopsided. It is a linear molecule, O=C=O, but carbon has 6 protons and oxygen has 8, so oxygen pulls the shared electrons closer. The oxygen ends sit slightly negative and the carbon centre slightly positive, and a free electron has something to grab onto. Every molecule vibrates from heat anyway; this charge imbalance is what lets CO₂ vibrate much harder on demand.

The molecule can only sit in specific vibration states: gentle (v=0), vigorous (v=1), more vigorous still (v=2). The step between v=0 and v=1 is where a CO₂ laser stores its energy.

And then the drop

A molecule at v=1 cannot gradually wind down to v=0. It drops, the way you fall off a step. One moment it is vibrating vigorously, the next it is not.

Energy has to be conserved, so the difference has to go somewhere, and it leaves as a photon carrying exactly that much: 0.117 eV, which is 10.6 μm infrared. That number is not a design choice. It is the size of the gap.

A laser head on its gantry cutting a curved line into a sheet of MDF, with a single bright orange point of light where the invisible beam meets the board.
A CO₂ machine cutting MDF. At 10.6 μm there is nothing to see between the head and the board, so the only evidence the beam exists is the bright point where it lands and the line it has already cut.

The interesting part: the wavelength is the crystal

A diode laser emits 450 nm blue because gallium nitride has a band gap of 2.75 eV. That is not a setting, a mode or a firmware value. It is the atomic structure of the semiconductor. Change the wavelength and you have changed the crystal.

Think of materials as electron parking lots. In a metal the lot is half full and electrons move anywhere, any time, which is why metals conduct. In an insulator the lot is completely full with a huge wall around it, so nothing moves. A semiconductor is full but the wall is short enough that electrons can occasionally get over it. That wall is the band gap, and in GaN it stands 2.75 eV tall.

What the diode part means

The chip is about 1 mm on a side, with two wires and mirrors formed by cleaving the crystal so the polished edges reflect. To make it a diode you dope the semiconductor with two different impurities. The n-type zone has extra electrons; the p-type zone has missing ones, and those empty spaces behave like positive charges, so they get called holes. They move through the material as electrons hop from spot to spot.

That p-n junction is the diode, and diode just means two terminals. Current flows one way and stops the other. When such a junction emits light it is an LED; add mirrors so it lases and it is a diode laser. Same device.

Apply voltage and electrons flood the n side, holes the p side, and they meet at the junction. An electron falls from the high-energy conduction band into a low-energy hole, and it cannot ease its way down, it drops. That 2.75 eV difference leaves as a 450 nm blue photon.

A diode laser head on a gantry with a visible blue beam running from the nozzle down to a thin board, throwing smoke and a blue glow across the work surface.
A diode laser engraving a length of wood. 450 nm sits inside the range your eyes register, which is why this is the one laser here whose beam you can watch travel: that blue column is the 2.75 eV photons on their way down.

The interesting part: metres of amplifier, and it can pulse

Every other laser here amplifies light over centimetres or millimetres. A fiber laser does it over metres, because the gain medium is a coil of optical fiber that might run 1 m or 20 m inside the housing. A photon crossing all of that meets far more excited ions on the way, so the amplification is enormous.

The same shape gives it the other thing that matters: surface area. Heat spreads along metres of fiber instead of piling up in a chip, so you can pump kilowatts in without melting anything. And you can switch the pump diodes on and off in nanoseconds, which is the whole reason fiber lasers mark metal. Short pulses beat thermal diffusion.

What doped with ytterbium means

The fiber has a core of ultra-pure glass about 10 μm across, a cladding of different glass about 125 μm across, and pump diodes shining into it. Mirrors at both ends are usually fiber Bragg gratings, microscopic ripples etched into the core itself.

Doping means replacing some of the glass's silicon atoms with ytterbium, maybe 1 in 10,000. Ytterbium is a rare earth with electrons in 4f orbitals that sit partly buried inside the atom, shielded by the outer electrons, which gives it very specific and very stable energy levels. Picture tiny light bulbs embedded through the glass, each one a photon factory waiting to be switched on.

Pump diodes at 915 nm or 976 nm shine into the cladding, and the light bounces around in there, crossing the core again and again. Each crossing, ytterbium ions absorb pump photons and their electrons climb to a higher 4f level. When one drops back it releases 1,064 nm infrared at 1.17 eV.

A brass-coloured coin lying on a dark machine bed with an intense blue-green bloom of light at the single point where a fiber laser is marking it.
A fiber laser marking the face of a coin. Nanosecond pulses put the energy in faster than the metal can conduct it away, so the mark forms in a spot narrower than a hair and the surface around it is left alone.

The interesting part: nothing here lases at 355 nm

A UV laser is the odd one out, because it does not generate UV. To lase at 355 nm you would need a material with an energy gap of exactly 3.5 eV, and the materials that fit are unstable, toxic or need extreme conditions.

So you cheat. Build a fiber laser at 1,064 nm, which we know how to do reliably, then multiply its frequency by three in a stack of crystals. Triple the frequency, divide the wavelength by three, triple the photon energy. A UV laser is a fiber laser wearing two crystals.

Why bright light changes colour

Light passing through a crystal pushes and pulls on the electrons in its atoms. Under ordinary light they wiggle smoothly at the same rhythm as the incoming wave and re-emit the same colour. Red in, red out. Gentle rocking of a spring.

Now focus a fiber laser's output into a beam thinner than a hair. The force on those electrons becomes enormous, and they stop moving smoothly. They get jerked hard one way, snap back and get jerked again, like a spring slamming against its stops. And electrons moving in a jerky pattern emit several colours at once: the original 1,064 nm, plus double it at 532 nm green, plus triple it at 355 nm UV. That is what nonlinear means. The response is no longer proportional to the input.

Crystals like BBO, LBO and KTP have their atoms arranged lopsidedly, exposed on one side and buried on the other, so they respond unevenly and exaggerate the effect. Hence nonlinear crystals.

The two-crystal arithmetic

First crystal, doubling. Two infrared photons at 1.17 eV each push the same atom at the same instant, it wiggles at the combined rhythm, and one green photon at 2.34 eV comes out. 1.17 + 1.17 = 2.34. The two infrared photons are gone. They did not stick together like Lego, they were both spent on one atom.

Second crystal, mixing. Some infrared always survives the first pass, so now green and infrared hit the same atoms together, like two drummers at once. The atom responds at the combined rhythm. One green photon at 2.34 eV plus one infrared at 1.17 eV becomes one UV photon at 3.51 eV. That is sum frequency generation.

None of this is efficient. Roughly 50% converts on the doubling, then 30–40% on the mixing, so about 17.5% survives end to end. A 50 W fiber laser might yield 10 W of UV, with the rest becoming heat in the crystals. Add precision-cut crystals, active temperature control and alignment optics on top of a powerful fiber laser and you have the reason UV machines cost what they cost.

A figurine etched in frosted white inside a clear glass block, with a narrow pale beam track running down through the glass to a bright point on the top of its head.
A UV laser working inside a solid block of glass, forming a figurine below the surface. Glass stays transparent to this beam until the focus is tight enough to break it internally, which is why the damage sits where the focus is and not on the face the light passed through.

What comes out, and why

Output wavelength, photon energy and the transition that fixes it, per laser type
LaserOutputPer photonTransitionFixed by
CO₂10.6 μm infrared0.117 eVVibrational, in a gas molecule (nuclear motion)The gap between CO₂’s v=1 and v=0 vibration states
Diode450 nm blue2.75 eVElectronic, across a semiconductor band gapThe band gap of gallium nitride
Fiber1,064 nm near-infrared1.17 eVElectronic, in a rare-earth ion’s 4f orbitalsThe 4f energy levels of ytterbium
UV355 nm ultraviolet3.5 eVNone of its own. A fiber laser, frequency-tripledArithmetic: three times the fiber frequency

What to do with this

CO₂ stores energy in nuclear motion, which is why it matches organic materials so well. Same quantum mechanism on both sides of the cut.

Diodes store it in a semiconductor band gap. Cheap and compact, wrong wavelength for most materials.

Fiber stores it in rare-earth ions and can pulse in nanoseconds, which is what beats thermal diffusion in metal.

UV is a frequency-tripled fiber laser. High photon energy breaks bonds directly without bulk heating, at roughly a sixth of the efficiency and several times the price.

But why does an electron have to drop rather than ease down? Electrons and molecules cannot gradually lose energy, they have to suddenly jump from one state to another. What stops them releasing it slowly, like a ball rolling down a hill? And for that matter, where does the octet rule come from? Why 8 electrons? Who decided these numbers?

Why energy comes in jumps at all

This is the last why, and it is the one where even physicists eventually say the math works and nobody knows why reality is like this.

Look, you don't need this level

Seriously. You already have everything you need to understand why your CO₂ cuts wood and your diode does not. Stop here and you know more than 99% of people who own lasers.

But if you are still reading, you are probably the kind of person who cannot let go of why energy states have to be discrete, why an electron cannot just ease its way down, or what is so special about the number 8.

All of those have the same answer: because electrons are waves, waves trapped in a confined space can only exist in specific patterns, and those patterns have specific energies. An electron can no more take an in-between energy than a guitar string can vibrate at a frequency between its allowed notes.

If that is enough, great, you are done. Fair warning if it is not: this gets into quantum mechanics. Not the math (I'm not a sadist), the concepts. It is weird and it will make you uncomfortable, which is normal, because it made the physicists who discovered it uncomfortable too.

Standing waves in a baking pan

Fill a baking pan with water and slosh it back and forth at random speeds. The water jiggles, waves bounce off the sides and interfere, and mostly nothing happens. Find exactly the right rhythm and you get huge standing waves instead: water piling at the edges, crashing down the middle, perfectly synchronised and building with every push.

That is a mode, a wave pattern that reinforces itself because it fits the space. The pan's size decides which frequencies work. Push slightly off that rhythm and the water fights you, because your push is sometimes in phase and adding energy and sometimes out of phase and taking it back. The energy sloshes between the water and your hand instead of accumulating. Hold onto that, because it is the entire explanation for why your diode struggles.

Guitar strings do the same thing. One half-wavelength fits the string and you get the fundamental; two fit and you get the second harmonic; three and you get the third. Anything in between cancels itself out, because only patterns that satisfy the fixed ends can survive. Organ pipes, same deal.

The pattern to hold onto

Confine a wave to a space with boundaries and only certain patterns can exist. Everything else destructively interferes and disappears. This is not an analogy for quantum mechanics. This is quantum mechanics.

Electrons are waves

Here is where it gets uncomfortable, because everything above applies to electrons. They are not little balls. They are waves.

The double-slit experiment settled it. Fire electrons through two narrow slits and, if they were particles, you would get two bright stripes. What you actually get is an interference pattern of alternating bright and dark bands, exactly like water waves passing through two gaps and overlapping.

And it holds even when you fire them one at a time, so slowly that only one electron is ever in the apparatus. The pattern still builds up dot by dot. Each electron interferes with itself, which means it is not going through one slit or the other, it is a wave going through both. Try to measure which slit and the pattern vanishes. They act like particles when you look and waves when you do not.

This is measurable, repeatable physics rather than philosophy. Electrons are waves, specifically waves of probability describing where one might be found if you measured it.

So if electrons are waves and atoms are the spaces confining them, atoms are tiny three-dimensional organ pipes. Only certain electron wave patterns can exist around a nucleus; the rest collapse immediately. Those stable patterns are what we call orbitals. Not orbits, because nothing is travelling in a circle.

Where discrete energy levels come from

Now the question answers itself. v=0, v=1, v=2 for molecular vibrations, discrete electron energy levels, specific photon wavelengths: they are all standing wave patterns, and only certain patterns fit.

A C-O bond is a spring with a nucleus on each end, except the spring is the electron cloud and the nuclei have wave properties too. v=0 is the fundamental, the lowest standing wave the bond supports. v=1 is the first harmonic, a more vigorous pattern where the nuclei swing further. v=0.5 cannot exist for the same reason a guitar string cannot vibrate between its fundamental and its first harmonic. The pattern does not fit, so it interferes with itself and dies.

Level 43.5 eVGapLevel 32.75 eVGapLevel 21.17 eVGapLevel 10 eV (ground)e⁻No Level 2.5 exists
The allowed levels, and the gaps between them. Push the electron up and it has to land on a rung; there is no level 2.5 to stop at, which is why a photon either carries exactly the right energy or does nothing at all.

Where the number 8 comes from

Solve the wave equation for electrons around a nucleus and only certain 3D patterns come out stable: spheres, dumbbells and more complicated shapes.

First shell: one spherical pattern (1s), 2 electrons.

Second shell, where chemistry happens: one spherical pattern (2s) and three dumbbell patterns (2p). Four patterns, 2 electrons each, 8 total.

Shell 2 supports exactly four stable wave patterns because that is what the geometry of fitting waves around a nucleus in 3D allows. Not three, not five. That is where the octet rule comes from, and it is geometry rather than a rule anyone wrote down.

Why only 2 per pattern? The Pauli exclusion principle: no two electrons can be in exactly the same state. But electrons have a property called spin, which is not literal spinning (they are waves) but is real and measurable, and it comes in two options. So each orbital takes one of each, and that is it. A third has to find a different pattern or go up a shell.

An atom with every pattern filled is stable, and one with gaps is reactive. Carbon has 6 electrons and needs 4 more to complete shell 2, so it shares with oxygen, hydrogen and other carbons, and that is how you get cellulose and lignin. Oxygen has 8 and needs 2, so it forms the C-O and O-H bonds your CO₂ laser is aimed at. Neon has 10, every pattern full, and bonds with nothing at all.

On resonance, energy is trapped. Off resonance, it comes back out.

Back to the baking pan, because this is the payoff. When a photon's frequency matches a transition between allowed states, each push adds energy to the standing wave. A 10.6 μm photon oscillates at exactly the v=0 to v=1 frequency of a C-O bond, so every photon that arrives pushes at the right rhythm. Energy accumulates in the vibrational mode, and with damping from collisions it cannot re-radiate fast enough, so it becomes heat. Temperature builds, bonds break, wood vaporises.

When the frequency does not match, the field still pushes on the electrons, just at the wrong rhythm. A 450 nm photon oscillates at 667 THz against the bond's 28 THz, roughly 24 times too fast. The electrons get shaken but out of phase with the driving field, and the oscillation they produce re-radiates most of the photon's energy straight back out. Elastic scattering. Light bouncing off. Maybe 1–5% couples into heat through random collisions, and the rest reflects or passes through.

Which is the whole guide, in one paragraph

Your 20 W diode struggles on light wood because most of its photons are off resonance for the C-O and C-H bonds that make up cellulose, so the energy sloshes back out. Only chromophores have wave patterns that match blue. Your 60 W CO₂ hits nearly every photon at the right frequency, energy gets trapped instead of re-radiated, and you are at ~90% absorption. That is the difference.

Why you cannot add power to fix a wavelength problem

One more quantum rule, and it is the one that makes the whole guide practical. Energy does not merely come in different amounts, it is quantized. Planck worked this out in 1900 trying to explain why hot objects glow: energy transfers in chunks, and the size of the chunk is locked to the frequency.

Which means you cannot save up small chunks to make a big one. Each photon interaction is independent. Either the chunk is big enough to cause the transition or it is not.

A C-C bond needs about 3.6 eV to break. A UV photon carries 3.5 eV and can do it directly. A CO₂ photon carries 0.117 eV. You could run a 60 W CO₂ against a 5 W UV and the UV would break C-C bonds while the CO₂ would not, and it has nothing to do with total power. Thirty CO₂ photons hitting the same bond do not pool their energy into one 3.5 eV event. They are thirty separate tiny interactions that each fail.

The transitions themselves are instantaneous for the same reason the levels are discrete: there is no in-between pattern to pass through, the way a guitar string cannot be halfway between two harmonics. When the drop happens the energy either becomes heat, spreading through the material as phonons, which is how cutting happens, or it becomes a photon, which is how lasers work.

What to do with this

You now have something most laser buyers do not, which is the actual reason a wavelength either works on a material or does not.

Next time you are looking at an unfamiliar material you do not have to guess. Look up what it is made of, find the energy gaps, match them to wavelengths. Five minutes instead of a stack of ruined test sheets.

And when someone shows you a spec sheet claiming a 30 W diode equals a 50 W CO₂, you know which questions to ask. What wavelength? What material? What bond energies?

Now when I review lasers, I ask about wavelength before I ask about power. When some company sends me a press release claiming their new 30W diode "rivals CO₂ performance," I order test materials. Because $600 taught me marketing doesn't understand quantum mechanics.

→See which marks your laser can actually make Computed verdicts per machine, material and mark type, with the reason attached to every one.

That is as deep as the physics goes. After this you are asking why math describes reality, and nobody knows.

The useful direction from here is outward, not back to the top. Take an actual material and check it. The material guide has a row per material with the shop reality and the physics reason behind it. Five minutes, the way the takeaway above says.

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