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Metal-coated mirrors are mirrors (optical reflectors) based on a thin metal coating, produced with an evaporation or sputtering technique. The metallic coating is placed on a substrate, which is often consisting of a glass, or possibly also of a metal. Common metal coatings consist of aluminum, silver or gold; less common are copper, chrome and various nickel/chrome alloys.
Often, the metal layer is covered with a thin layer or multiple layers of a dielectric material such as amorphous SiO2 (silica) or Si3N4 (silicon nitride), which protects the coating against oxidation (tarnish) and scratches. Such protected coatings are definitely more abrasion-resistant than uncoated ones, but still they tend to be more sensitive than dielectric mirrors. This implies that greater care is required for cleaning of metal-coated optics. Also, metallic mirrors are more or less sensitive to humidity and corrosive gases.
Multilayer protection coatings can also be used to enhance the reflectivity (see below); this leads to enhanced metal coatings. The resulting metal dielectric coating effectively combines the large bandwidth of a metallic mirror with the higher reflectivity and damage threshold of a dielectric mirror.
Broad Bandwidth, Low Chromatic Dispersion
A big advantage of metal-coated mirrors over dielectric mirrors is that the reflectivity is quite uniform over a wide spectral range and also quite insensitive to the angle of incidence and polarization. Also, metal-coated mirrors can be fabricated easily and are thus relatively cheap. Therefore, they are often used as general-purpose mirrors. Also, they are sometimes required for ultrashort pulses with ultrabroad bandwidth, where it is difficult to obtain sufficient reflection bandwidth from dielectric mirrors (although chirped dielectric mirrors nowadays also offer very large bandwidths). In that context, it also relevant that metal-coated mirrors exhibit very weak chromatic dispersion; the reflection phase-shift exhibits a very small wavelength dependence. This is useful, for example, for use as reference mirrors in white-light interferometers.
Metal-coated mirrors can also work for extremely long infrared wavelengths, e.g. up to 20 μm. In that region, it is difficult to work with dielectric mirrors, as dielectrics then exhibit strong absorption.
A disadvantage of metallic mirrors, when compared with dielectric mirrors, are the significant reflection losses. This limitation is of fundamental nature, as metals inevitably absorb some of the incident light (even if they are very pure). As a consequence, the reflectivity is limited, e.g. to roughly 98% for protected silver mirrors. Another consequence is the relatively low optical damage threshold: the absorbed light leads to heating, and as the heat is deposited in a quite thin layer, this can easily lead to damage. Both in terms of average power and peak power, the damage threshold is low. For high average powers, substantial thermal lensing and thermal beam distortions can arise from heating effects even well below the damage threshold.
The reflection losses may be reduced with dielectric multilayer coatings. Such enhanced coatings also lead to a correspondingly higher optical damage threshold. For example, the damage threshold of an enhanced coating silver mirror for nanosecond pulses from a 1064-nm YAG laser can be several J/cm2, whereas it may be only 0.5 J/cm2 for a simple protected silver mirror (and even much less for aluminum). For comparison, dielectric mirrors can stand several tens of J/cm2.
Partially Transmissive Mirrors
It is possible to obtain partial transparency of a metal coating by making it very thin. However, the losses are substantial, so that the sum of transmittivity and reflectivity is well below 1. It is more common to use dielectric mirrors for such applications, but partially transmissive metal-coated mirrors are used if a very high operation bandwidth is required and high power losses can be tolerated.
Aluminum coatings are used for the visible and ultraviolet spectral region, reaching reflectivities well above 90% in the visible but often below 90% in the UV.
Silver coatings are suitable for wavelengths from about 500 nm to 20 μm. Due to their lower losses, they also generally exhibit higher damage thresholds than aluminum mirrors.
Gold mirrors are similar, but can be used only for about 600 nm and longer wavelengths. Here, reflectivities well over 95% (sometimes around 99%) are achieved. It is possible, for example, to obtain an average reflectivity of 97% between 700 and 2000 nm with a protected gold mirror. Sometimes, an unprotected gold mirror is preferred in order to avoid any dispersion from a protective coating; this is possible as gold does not tend to get oxidized.
Gold-coated copper mirrors (sometimes fabricated with electrochemical techniques) can be used with high-power infrared lasers, such as CO2 lasers. Here, substantial amounts of heat can be tolerated due to the high thermal conductivities of gold and copper.
First Surface versus Second Surface Metallic Mirrors
For a first surface mirror, the reflective coating is on the side of the incident light. The light only slightly penetrates the coating, but does not reach the substrate.
Second surface mirrors have the reflecting coating on the other side of the substrate, so that the coating can be better protected. The light propagates through the substrate before and after the reflection. This type of mirror is also common for household applications. In technical applications, problems can arise from the Fresnel reflection at the first surface (which can lead to ghost images, for example, and to some power losses), and in some applications from the chromatic dispersion of the glass.
See also: laser mirrors, dielectric mirrors, chromatic dispersion, infrared light, neutral density filters
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