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Laser Safety

  • Article Content:

    In the early 1960s, the laser was an invention looking for an application. Not so any more today, lasers have myriad uses:

    • Checkout counter scanners
    • Consumer devices -- CD and videodisk players, laser printers, laser pointers, etc.
    • Industrial -- imaging, welding, cutting, drilling, trimming, scoring
    • Surgery

    In other words, the laser now is a common tool. Like most other tools, lasers are capable of causing injury to their operators and others, if improperly used.

    Elements of Laser Safety

    Light

    First and foremost, the laser is a device that produces light, hence the acronym LASER, which stands for Light Amplification by Stimulated Emission of Radiation. The word "light" evokes in us thoughts of visible light, but most light is not visible: our eyes respond to only a narrow band of wavelengths, from about 400 nanometers (nm) in the violet, to about 760 nm in the red. Yet there is ultraviolet light (UV C wavelengths shorter than 400 nm) and infrared light (IR C wavelengths longer than 760 nm), which lasers and other light sources produce, but which cannot be seen.

    Laser light

    Laser light has several notable qualities, some of which are unique:

    • Laser light is monochromatic, meaning that it is all of one wavelength.
    • Laser light is highly directional, in a tight beam.
    • The laser beam is highly collimated, i.e., very "parallel."
    • Because of the directionality and collimation, laser beams can be very powerful.
    • Laser beams tend to be small in diameter, often 1 mm or less.

    The Human Eye

    Let's look at the human eye: The cornea is the main focusing element, and the lens performs fine focusing duties. The space between the cornea and lens is filled with a watery liquid known as the aqueous humor, and the interior of the eyeball is filled with the jelly-like vitreous humor. The retina is the screen upon which the cornea and lens project an image of the outside world. The fovea is the seat of sharp vision. The retina is connected to the brain by the optic nerve. Signals generated in the retina are transmitted by the optic nerve to the brain, which interprets these signals as vision. The cornea, aqueous humor, lens, and vitreous humor are called the ocular media. They are the stuff through which light must pass to reach the retina.

    Obviously, light must reach the retina, and the retina must respond to it, in order for us to see the light. In order for light to reach the retina, the ocular media must be transparent to it. Here we see that the ocular media are transparent to visible light (surprise!).

    The lens absorbs UV, and the older we get, the more the UV cutoff extends to the longer wavelengths. Babies and young children can in fact see a ways into the UV, but the lens yellows with age and by the time we are adults, most of us have lost that ability. UV lasers thus are not retinal hazards, although they can be hazardous to the eye in other ways.

    But note how far the transparency of the ocular media extends into the infrared (IR) C all the way out to 1400 nm, in varying degree. The retina normally does not respond to wavelengths much longer than about 760 nm, so this light is invisible, even though it reaches the retina. This creates special hazards, which we will discuss later.

    This wavelength region, 400 nm - 1400 nm, is called the retinal hazard region.

    Laser Hazards

    The rated power of a laser often belies the hazards of the beam. For example, to the layman a power of ten Watts seems trifling -- barely enough to make a night-light. Yet, ten Watts in a 1-mm beam provides an irradiance greater than a thousand Watts/cm2, which can ignite flammable materials and cause severe skin burns. If the wavelength of the light is within the retinal hazard region it can reach the retina of the eye, and the high degree of collimation, which is characteristic of a laser beam, creates a special hazard.

    Recalling basic geometric optics, we remember that a parallel beam of light that enters a converging optical element, such as the cornea/lens focusing element of the eye, will be focussed down to a geometric point in the focal plane. This of course concentrates all the power in the beam into an infinitesimal spot, and results in an infinite irradiance.

    The cornea/lens is not aberration-free, and there is diffraction from the iris, so the spot on the retina is not infinitesimal C but it is very small: in a well-corrected eye, a laser beam can produce a spot 20 :m diameter on the retina. Such a spot has an area about 3 x 10-6 cm2.

    Thus, even a low power laser can produce a surprising retinal irradiance. Intrabeam viewing (i.e., the laser beam enters the eye directly) of a 1 mW (0.001 W) laser results in a retinal irradiance more than 300 W/cm2! Compare this to the 10 W/cm2 image of the sun on the retina of a person who views the sun at noon on a bright summer day.

    The optical gain of the eye for a highly collimated beam, which is the ratio of the area of the retinal image to the area of the pupil of the eye, is 105. This is why lasers in the retinal hazard region are capable of causing retinal damage.

    Damage Mechanisms

    Although it is tempting to compare the focussing action of the cornea/lens to that of a simple burning glass, other mechanisms may damage the retina:

    • Thermal
    • Photochemical
    • Mechanical

    Thermal is easiest to comprehend, because it is like the burning glass. Simply put, the irradiance is so high that the illuminated area on the retina becomes overheated and a burn results. There is a threshold for this type of damage, and repeated sub-threshold exposures are not cumulative, provided the retina has time to cool between them.

    Photochemical damage is more likely at the shorter visible wavelengths, peaking at about 440 nm. Repeated exposures within about a 24-hour period are cumulative.

    Mechanical damage results from acoustic shock waves generated by very short pulses. Less is known about this mechanism, but research is ongoing.

    It is important to realize that these mechanisms may act synergistically, in ways that are not completely understood.

    Near-IR lasers, 760 - 1400 nm, present special hazards. These wavelengths are in the retinal hazard region, but they are invisible. Thus stray beams and reflections cannot be seen, and might be detected only as the result of an injury. Many serious retinal injuries have been caused by accidental exposure to near-IR laser beams.

    Non-retinal Laser Hazards

    The high irradiance or radiant exposure in an unfocussed laser beam can cause severe injury to the cornea and to other body tissues.

    ADDITIONAL SAFETY RESOURCES

    Laser Institute of America (LIA)

    12001 Research pkwt, STE 210
    Orlando, FL 32826
    Phone: 407-380-1553
    Toll Free: 1-800-34LASER

    American National Standards Institute

    ANSI Z136.1, American National Standard for the safe Use of Lasers
    (Available through LIA)

    International Electro-technical Commission

    IEC 60825-1, Edition 1.2
    Safety of laser products -
    Part 1: Equipment classification, requirements and user's guide.
    (Available through LIA)

    Center for Devices and Radiological Health

    21 CFR 1040.10 - Performance Standards for Light-Emitting Products

     

    US Department of Labor - OSHA

    Publication 8-1.7 - Guidelines for Laser Safety and Hazard Assessment

     

    Laser Safety Equipment

    Laurin Publishing
    Laser safety equipment and Buyer's Guides

     

     

    Haas Laser Technologies, Inc. recommends that laser users investigate any local, state or country requirements as well as facility or building requirements that may apply to installing or using a laser or laser system.

     

     

     

     

  • Article Picture:
  • Authors : Michael Scaggs, Gilbert Haas
  • Last Updated Date: 2025-02-06
  • Hits: 672

Technical Supplement: Cu/Ni/Au Mirrors

  • Article Content:

    Haas Laser Technologies, Inc is one of the world’s leading suppliers of metal mirrors for a wide variety of industrial laser applications. Advanced production techniques and specialized precious metal deposition processes have enabled the company to develop a wide variety of sizes along with convex, concave, cylindrical and aspheric curvatures. Internal water cooling is also available.

    SUBSTRATE

    Copper is the prime metal substrate employed for mirrors used in high-power C.W. and pulsed infra-red lasers. Its excellent thermal properties give long life-times and provide reliable performance in industrial applications.

    Bare copper, like most bulk metals, has a grain structure in the surface due to its natural crystalinity. This grain structure shows the grain boundaries which are subject to a thermoelastic mechanism failure when under irradiation known as “slip banding”. Under this condition, grain boundaries on the surface slip, increasing the localized absorption, swiftly leading to catastrophic melting, cratering, roughening, and destruction of the optic. This happens way before the mirror damages.

    “Slip banding” is the limiting damage mechanism in mirror substrates and why the material should be chosen for it’s thermoelastic properties and not it’s thermal properties. It is the thermoelastic weakness in the grain structure of crystalline materials that leads to optic damage.

    COATINGS

    “The use of microdispersed polycrystalline materials between the reflective layer and the metal base significantly improves the stability of metal optics…” (Prokohorov “ Laser Heating of Metals”, 1990). Prokohorov’s theory of damage to optical materials from “slip banding” has been widely demonstrated to show that the limiting factor is the crystalline surface structure. If the surface structure contains no grain boundaries, the limitation imposed on the mirror by slip banding is removed, and the mirror is free to work at much higher powers.

    Haas Laser Technologies, Inc’s use of amorphous nickel plating, gives a surface layer free from grain boundaries and crystalline features and hence no possibility of damage by “slip banding”. This enables the highest possible damage thresholds for pulsed and CW lasers. The amorphous nickel is then gold plated giving an exceptionally smooth surface which never peels or flakes even when burnt or scratched. There is no danger of immediate catastrophic failure as with nearly all other mirrors. Mirrors can therefore be replaced when convenient.

    In addition, gold is totally inert to all aqueous and organtic liquids and gases over long periods of exposure. Mirrors can be stored for many years without loss in performance. Bare copper absorbs sulfur and chlorine like a sponge causing tarnishing and some loss of reflectance in industrial environments.

    POLISHING

    Metals can be difficult to polish. Soft metals such as copper can be particularly problematic in achieving good surface form and polish quality. The very best surface form and finish are still only achievable with traditional polishing techniques.

    A secondary method to polishing is diamond turning. Diamond turned mirrors exhibit lower damage thresholds, have rougher surfaces, and have more scatter. In addition, they tend to project “Target Patterns” and show ripple marks common with diamond machining.

    Talysurf measurements at the National Physical Laboratory, and electron Microscopy measurements at several universities have shown conforming surface roughness results on Haas Laser Technologies, Inc’s polished optics to be between 5-10 Angstroms RMS. This can be compared to the very best diamond turned surfaces of between 50 – 100 Angstroms.

    CW LASER DAMAGE

    Copper baser mirrors have long been the mirror of choice for high power CW and pulsed lasers. Although widely studied, values for the Laser Induced Damage Threshold (LIDT) have been inconsistent, and a variety of damage mechanisms have been postulated.

    Reliable damage thresholds have been established in conjunction with the University of Surrey, Lazer Zentrum Hannover, and several research institutions over a two-year period to investigate the physical processes involved.

    The most useful and fundamental result is that LIDT in CW lasers is related to the diameter of the irradiated area and the power.

    LIDT = P/D (P = laser power in watts, D = spot size in mm)

    To establish whether the LIDT value is exceeded in a specific system, one needs simply to know the maximum power used, and divide by the beams diameter.

    The LIDT for Haas Laser Technologies, Inc’s Cu/Ni/Au optics is 4000 W/mm.

    Some comparisons are: Fresh bare copper 2500 W/mm

    Gold coated Silicon 600-800 W/mm

    The value of 4000W/mm as LIDT for a Haas Laser Technologies, Inc’s Cu/Ni/Au type mirror has been obtained with a wide variety of spot sizes and powers. The relationship is remarkably linear, allowing LIDT’s to be accurate for any combination of laser power and beam diameter.

    PULSED LASER DAMAGE

    From a theoretical standpoint it is difficult to account for pulsed laser damage to bare copper mirrors to occur strictly from heating effects. Even taking into account non-linearity in the physical constants of the metal, catastrophic damage by heating and melting is not attributable as a result of the intrinsic absorption of the copper substrate.

    One obvious explanation of pulsed laser damage is that defects such as scratches and digs from polishing that act as damage initiation sites. This can be seen in variations in pulsed LIDT values.

    Haas Laser Technologies, Inc’s chemical polishing enables mirror surfaces to be free from residual features like scratches and digs. This process produces a typical surface roughness 5 Angstroms. In addition, there are no repetitive spatial features such as turning lines like in diamond turned optics which introduce beam scatter.

    Pulsed damage thresholds of copper mirrors are measured to be typically between

    6.4 – 9.6 J/cm2. Silicon is also measured to be within the same range. Haas Laser Technologies, Inc’s Cu/Ni/Au mirrors have been independently measured to be

    46.7 J/cm2. This is 10 times higher than copper and silicon.

    *Based on a 80ns laser pulse

    REFLECTIVITY

    Gold is totally inert to all aqueous and organic liquids over long periods of exposure.

    This means that there is no loss in reflectance over time as compared to copper and silicon based mirrors. Typical reflectance for Cu/Ni/Au mirrors are as follows:

     

    10.6um (CO2) >99.0%.

    1.064nm (Nd:YAG) >98.5%

    632.8nm (HeNe) >90%

    (Goldmax enhanced coatings are also available for internal resonator optics which provide a reflectivity of >99.8%)

    POLARIZATION

    Chemically deposited gold coatings have almost unmeasurable phase shift. Therefore, many mirrors can be used in a system without making the polarization elliptical. Gold coated mirrors can be used with any wavelength or angle of incidence. Hence, there is no need to choose a mirror optimized for a very narrow set of conditions.

    INTERFEROMETRY AND TESTING

    There is a long history and evolution of mirror testing techniques starting from the manufacture of telescopes and astronomical reflectors. We, at Haas Laser Technologies, Inc have adapted and modified these techniques for modern day laser mirrors.

    In the early stages of manufacture, a spherometer is used which can determine accuracies of 1 fringe over a 150mm diameter. A Fizeau interferometer in used on finished mirrors to image the wave front distortion in a double pass configuration and to measure the radius of curvature directly. Calibration results using the Fizeau test along with Ronchi and Foucault tests are compared to that of independent tests performed by the National Physical Laboratory London.

    BENEFITS

    These are a few benefits of Cu/Ni/Au mirrors.

    • High resistance to high power industrial lasers.
    • No effect on beam divergence or mode.
    • No effect on beam polarization.
    • Excellent reflectivity.
    • Rugged to withstand cleaning, debris, and fumes.

    Comparison between gold plated copper –vs- silicon mirrors:

    Specification Copper Base Silicon Base

    Damage Threshold 4000 W/mm 800 W/mm

    Phase Shift <0.5 Deg. 2-6 Deg.

    Reflectivity 99% 99.2+

    Coating Adhesion Never peels or flakes Fails Catastrophically

    Wavelength/ Incidence Not Important Needs to be specified

    Environmental Inert to all chemicals Sensitive to environment

     

     

  • Article Picture:
  • Authors : Michael Scaggs, Gilbert Haas
  • Last Updated Date: 2014-09-19
  • Hits: 573