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Krypton fluoride laser

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A krypton fluoride laser (KrF laser) is a particular type of excimer laser,[1] which is sometimes (more correctly) called an exciplex laser. With its 248 nanometer wavelength, it is a deep ultraviolet laser which is commonly used in the production of semiconductor integrated circuits, industrial micromachining, and scientific research. The term excimer is short for 'excited dimer', while exciplex is short for 'excited complex'. An excimer laser typically contains a mixture of: a noble gas such as argon, krypton, or xenon; and a halogen gas such as fluorine or chlorine. Under suitably intense conditions of electromagnetic stimulation and pressure, the mixture emits a beam of coherent stimulated radiation as laser light in the ultraviolet range.

KrF and ArF excimer lasers are widely incorporated into high-resolution photolithography machines, one of the critical tools required for microelectronic chip manufacturing in nanometer dimensions. Excimer laser lithography[2][3] has enabled transistor feature sizes to shrink from 800 nanometers in 1990 to below 45 nanometers in 2010.[4]

Theory

A krypton fluoride laser absorbs energy from a source, causing the krypton gas to react with the fluorine gas producing the exciplex krypton fluoride, a temporary complex in an excited energy state:

2 Kr + F
2 → 2 KrF

The complex can undergo spontaneous or stimulated emission, reducing its energy state to a metastable, but highly repulsive ground state. The ground state complex quickly dissociates into unbound atoms:

2 KrF → 2 Kr + F
2

The result is an exciplex laser which radiates energy at 248 nm, near the ultraviolet portion of the spectrum, corresponding with the energy difference between the ground state and the excited state of the complex.

Applications

The most widespread industrial application of KrF excimer lasers has been in deep-ultraviolet photolithography[2][3] for the manufacturing of microelectronic devices (i.e., semiconductor integrated circuits or “chips”). From the early 1960s through the mid-1980s, Hg-Xe lamps had been used for lithography at 436, 405 and 365 nm wavelengths. However, with the semiconductor industry’s need for both finer resolution (for denser and faster chips) and higher production throughput (for lower costs), the lamp-based lithography tools were no longer able to meet the industry’s requirements. This challenge was overcome when in a pioneering development in 1982, deep-UV excimer laser lithography was demonstrated at IBM by K. Jain.[2][3][5] With phenomenal advances made in equipment and technology in the last two decades, modern semiconductor electronic devices fabricated using excimer laser lithography now total more than $400 billion in annual production. As a result, it is the semiconductor industry view[4] that excimer laser lithography (with both KrF and ArF lasers) has been a crucial factor in the predictive power of Moore’s law. From an even broader scientific and technological perspective: since the invention of the laser in 1960, the development of excimer laser lithography has been highlighted as one of the major milestones in the 50-year history of the laser.[6][7][8]

The KrF laser has been of utility in the nuclear fusion energy research community in inertial confinement experiments. This laser has high beam uniformity, short wavelength, and the feature of an adjustable spot size.

In 1985 the Los Alamos National Laboratory completed a test firing of an experimental KrF laser with an energy level of 1.0 × 104 joules. The Laser Plasma Branch of the Naval Research Laboratory completed a KrF laser called the Nike laser that can produce about 4.5 × 103 joules of UV energy output in a 4 nanosecond pulse. Kent A. Gerber was the driving force behind this project. The latter laser is being used in laser confinement experiments.

This laser has also been used to produce soft X-ray emission from a plasma, through irradiation by brief pulses of this laser light. Other important applications include manipulating of various materials such as plastic, glass, crystal, composite materials and living tissue. The light from this UV laser is strongly absorbed by lipids, nucleic acids and proteins, making it useful for applications in medical therapy and surgery.

Safety

The light emitted by the KrF is invisible to the human eye, so additional safety precautions are necessary when working with this laser to avoid stray beams. Gloves are needed to protect the flesh from the potentially carcinogenic properties of the UV beam, and UV goggles are needed to protect the eyes.

See also

References

  1. ^ Basting, D. and Marowsky,G., Eds., Excimer Laser Technology, Springer, 2005.
  2. ^ a b c Jain, K.; Willson, C.G.; Lin, B.J. (1982). "Ultrafast deep UV Lithography with excimer lasers". IEEE Electron Device Letters. 3 (3): 53–55. doi:10.1109/EDL.1982.25476.
  3. ^ a b c Jain, K. “Excimer Laser Lithography”, SPIE Press, Bellingham, WA, 1990.
  4. ^ a b La Fontaine, B., “Lasers and Moore’s Law”, SPIE Professional, Oct. 2010, p. 20.
  5. ^ Basting, D., et al., “Historical Review of Excimer Laser Development,” in Excimer Laser Technology, D. Basting and G. Marowsky, Eds., Springer, 2005.
  6. ^ American Physical Society / Lasers / History / Timeline
  7. ^ SPIE / Advancing the Laser / 50 Years and into the Future
  8. ^ U.K. Engineering & Physical Sciences Research Council / Lasers in Our Lives / 50 Years of Impact
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