CO_2 lasers (original) (raw)

Definition: infrared lasers based on a gas mixture in which light is amplified by carbon dioxide molecules

Alternative term: carbon dioxide lasers

Category: laser devices and laser physics

• gas lasers
  • molecular lasers
    * CO2 lasers
    * CO lasers
    * nitrogen lasers
    * acetylene lasers
    * hydrogen-fluoride lasers

Related: gas lasersmolecular laserslaser markinghigh-power laserssolid-state lasersinfrared optics

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Contents

What are CO2 Lasers?

The CO2 laser (carbon dioxide laser) is a molecular gas laser with emission in the long-wavelength infrared spectral region. It is based on a gas mixture as the gain medium, which contains carbon dioxide (CO2), helium (He), nitrogen (N2), and possibly some hydrogen (H2), oxygen (O2), water vapor and/or xenon (Xe). Such a laser is electrically pumped with a gas discharge, which can be operated with DC current, with AC current (e.g. 20–50 kHz) or in the radio frequency (RF) domain.

Although direct excitation of CO2 molecules into the upper laser level is possible, it has proven to be most efficient to use a resonant energy transfer from nitrogen molecules. Here, nitrogen molecules are excited by the electric discharge into a metastable vibrational level and transfer their excitation energy to the CO2 molecules when colliding with them. The excited CO2 molecules then largely participate in the laser transition. Helium serves both to depopulate the lower laser level and to remove the heat. Other constituents such as hydrogen or water vapor can help (particularly in sealed-tube lasers) to reoxidize carbon monoxide (CO, formed in the discharge) to carbon dioxide.

Figure 1: Schematic setup of a sealed-tube carbon dioxide laser. The gas tube has Brewster windows and is water-cooled.

Spectral Lines

CO2 lasers typically emit at a wavelength of 10.6 μm, but there are dozens of other laser lines in the region of 9–11 μm (particularly at 9.6 μm). This is because two different vibrational states of the CO2 molecules can be used as the lower level, and for each vibrational state, there is a substantial number of rotational states, leading to many sub-levels. Dipole transitions (the only ones with a relatively high strength) are possible with ($\Delta J$) = ±1, where ($\Delta J = 1$) (R branch) leads to higher photon energies (shorter wavelengths) and ($\Delta J = -1$) (P branch) to lower energies:

• Transitions of the stronger band, involving one of the two possible final vibrational levels, have their P branch around 10.6 μm, with P20 being the dominant transition, and the R branch around 10.2 μm.
• Transitions of the other band have the P branch around 9.6 μm and the R branch around 9.3 μm.

With a suitable wavelength tuning element in the laser resonator, a CO2 laser can be made to lase on one of more than a dozen transitions with relatively closely spaced wavelengths in each branch, but continuous wavelength tuning is not possible due to the discrete rotational states of the molecules. Without a wavelength-selective element in the resonator, one may obtain simultaneous lasing on a few transitions, or occasional jumps to other transitions during operation.

While most commercially available CO2 lasers emit at the standard wavelength of 10.6 μm, there are devices which are specially optimized for other wavelengths such as 10.25 μm or 9.3 μm, which are far better suited for certain applications for example in laser material processing because that radiation is much more absorbed in certain materials (e.g. polymers). For making such lasers and for using their radiation, one may require special infrared optics, as standard transmissive 10.6-μm optics may e.g. exhibit too strong reflections.

All CO2 laser emission lines can be considered to be in the long-wavelength infrared region, which is part of the mid-infrared region according to ISO 20473:2007.

Output Powers and Efficiency

In most cases, average output powers are between some tens of watts and many kilowatts. The power conversion efficiency can be around 10% to 20%, i.e., it is higher than for most gas lasers (due to a particularly favorable excitation pathway), also higher than for lamp-pumped solid-state lasers, but lower than for many diode-pumped lasers.

Due to their high output powers and long emission wavelengths, CO2 lasers require high-quality infrared optics, often made of materials like zinc selenide (ZnSe) or zinc sulfide (ZnS).

Due to their high powers and high drive voltages, CO2 lasers raise serious issues of laser safety. However, their long operating wavelength makes them relatively eye-safe at low intensities, as the light cannot get to the retina, the eye's most sensitive part.

CO2 Laser Types

The family of CO2 lasers is very diverse:

• For laser powers between a few watts and a several hundred watts, it is common to use sealed-tube or no-flow lasers, where the laser bore and gas supply are contained in a sealed tube. Waste heat is transported to the tube walls by diffusion (with a quite helpful effect of the helium) or a slow gas flow. Such lasers are compact and rugged, and easily reach operation lifetimes of several thousand hours or more. Here, one needs to employ methods for continuously regenerating the gas — in particular, for counteracting the dissociation of CO2 by catalytic re-oxidation of CO. The beam quality can be very high.
• High-power diffusion-cooled slab lasers (not to be confused with solid-state slab lasers) have the gas in a gap between a pair of planar water-cooled RF electrodes. The excess heat is efficiently transferred to the electrodes by diffusion, if the electrode spacing is made small compared with the electrode width. For efficient energy extraction, one often uses an unstable resonator with output coupling at the side of a highly reflecting mirror. Several kilowatts of output are possible in conjunction with reasonable beam quality.
• Fast axial flow lasers and fast transverse flow lasers are also suitable for multi-kilowatt continuous-wave output powers and high beam quality. The excess heat is removed by the fast-flowing gas mixture, which passes an external cooler (heat exchanger) before being used again in the discharge. The gas can be continuously regenerated and occasionally replaced. Transverse flow lasers reach highest output powers, but typically with lower beam quality.
• Transverse excited atmosphere (TEA) lasers have a very high (about atmospheric) gas pressure. As the voltage required for a longitudinal discharge would be too high, transverse excitation is done with a series of electrodes along the tube. TEA lasers are operated in pulsed mode only, as the gas discharge would not be stable at high pressures. They often produce average output powers below 100 W, but can also be made for powers of tens of kilowatts (combined with high pulse repetition rates).
• There are gas dynamic CO2 lasers (a kind of chemical lasers) for multi-megawatt powers (e.g. for anti-missile weapons), where the energy is not provided by a gas discharge but by a chemical reaction in a kind of rocket engine.

These concepts lead to quite different laser architectures, with specific strengths and weaknesses concerning output power potential, beam quality, gas consumption and device lifetime.

Applications of CO2 Lasers

CO2 lasers are widely used as industrial lasers for laser material processing, in particular for

• cutting and structuring plastic materials, wood, die boards, glass pieces, etc., which exhibit high absorption at 10.6 μm, mostly applying moderate power levels of 20–200 W
• cutting, welding and cladding metals such as stainless steel, aluminum or copper, applying multi-kilowatt powers
• laser marking of various materials
• laser hardening e.g. of machine parts made of steel
• laser soldering in electronics
• laser 3D printing of polymer materials

Other applications include laser surgery (including ophthalmology), range finding (LIDAR) and spectroscopy.

Competition with Solid-state Lasers

CO2 lasers used for laser material processing (e.g. welding and cutting of metals, or laser marking) are in competition with solid-state lasers (particularly YAG lasers and fiber lasers) operating in the 1-μm wavelength regime. These shorter wavelengths have the advantages of more efficient absorption in a metallic workpiece and the potential for beam delivery via fiber cables. (There are no optical fibers for high-power 10-μm laser beams, since there are no suitable materials with very high transparency in that region.) Besides, 1-μm beams can be more tightly focused, provided that the beam quality is high. However, the latter potential normally cannot be realized with high-power lamp-pumped lasers, and diode-pumped lasers tend to be more expensive. Concerning absorption, CO2 laser beams are actually quite favorable for certain materials like polymers and ceramics. Even when absorption is less favorable than for a solid-state laser, a CO2 laser may be preferred as a relatively cheap and robust solution. A substantial disadvantage, however, is that there are no high-power fiber cables for CO2 laser radiation.

CO2 lasers are still widely used in the cutting and welding business, particularly for parts with a thickness greater than a few millimeters, and their sales still make a substantial part of all global laser sales. This may to some extent change in the future due to the development of high-power thin-disk lasers and advanced fiber cables in combination with techniques which exploit the high beam quality of such lasers.

Frequently Asked Questions

This FAQ section was generated with AI based on the article content and has been reviewed by the article’s author (RP).

What is a CO2 laser?

A CO2 laser is a type of molecular gas laser that emits light in the long-wavelength infrared region, typically at 10.6 µm. Its active gain medium is a gas mixture containing carbon dioxide (CO2), which is energized by an electrical discharge.

How does a CO2 laser work?

CO2 lasers are electrically pumped. In the most efficient scheme, nitrogen molecules are excited by an electric discharge and then transfer their energy to CO2 molecules via collisions, causing a population inversion necessary for lasing.

What are the main applications of CO2 lasers?

CO2 lasers are widely used for industrial material processing, including cutting, welding, and marking of materials like plastics, wood, and metals. They also have applications in surgery and spectroscopy.

What is the typical emission wavelength of a CO2 laser?

The most common emission wavelength is 10.6 µm. However, CO2 lasers can be tuned to operate on dozens of other discrete emission lines in the spectral range between 9 µm and 11 µm.

What are the main types of CO2 lasers?

Common types include sealed-tube lasers for low to medium powers, fast axial or transverse flow lasers for multi-kilowatt outputs, diffusion-cooled slab lasers, and pulsed TEA (Transverse Excited Atmosphere) lasers.

How do CO2 lasers compare to fiber lasers for material processing?

CO2 lasers are often preferred for processing non-metallic materials like polymers, wood, and glass due to better absorption at their 10.6-µm wavelength. Fiber lasers (~1 µm) can be more effective for metals and allow beam delivery via flexible optical fibers.

Are CO2 lasers dangerous to the eyes?

Yes, they are. Although their long-wavelength radiation is blocked by the cornea and does not damage the retina, it can cause severe and permanent corneal burns. Therefore, appropriate safety precautions are essential.

Suppliers

Sponsored content: The RP Photonics Buyer's Guide contains 51 suppliers for CO2 lasers. Among them:

⚙ hardware

Coherent® Diamond C-Series CO2 lasers offer reliability with more than 50,000 operating hours, along with superior beam quality and stability. These lasers are ideal for a wide range of applications from marking and engraving to material processing. They are a compact option with an integrated RF power supply. Maximum output power ranges from 20 to 40 watts, and can be controlled through pulse width modulation (PWM).

⚙ hardware

LightMachinery is the world's leading manufacturer of Transversely Excited Atmospheric Carbon Dioxide (TEA CO2) lasers. Our laser team pioneered the development of TEA CO2 laser technology and has been designing carbon dioxide lasers and laser marking and drilling systems for over 30 years.

The LightMachinery IMPACT Series high power lasers are designed for 24/7 materials processing and drilling of non-metallic materials. These pulsed lasers are optimized for precision processing and drilling of non-metallic materials.

The LightMachineary LaserMark Series is the ultimate in marking reliability, from beer labels and gelcaps to miniature electronics components. These lasers are designed for on-line marking and coding, creating perfect, crisp images on your products 24/7.

Bibliography

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