With the continuous development of science and technology, the optical industry is also booming, and optical lenses are used more and more widely. Today, let's learn the specific content and working principle of the most common achromatic lens.
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An achromatic lens is a lens formed by cementing two optical components, a positive low refractive index and a negative high refractive index.
Compared to single-piece glass lenses, the cemented design of the double-piece lens provides the user with additional design freedom and further optimizes lens performance, so compared with the monolithic lens with equal diameter and focal length, achromatic lens has more obvious advantages.
Achromatic lens is made of concave and convex lenses made of two glasses with different optical properties. It is often used for convex lenses made of glass with small refractive index and large dispersion power, and concave lenses made of glass with large refractive index and small dispersion power.
Achromatic lenses generally can only superimpose the images and points of the two main colors of light that are considered to be the main ones, thereby eliminating the chromatic aberration of the two colors of light.
Chromatic aberration is caused by the difference in the dispersion and refractive index of light of different wavelengths in the glass, resulting in different focal points of light of different wavelengths, using the combination of different materials.
Achromatic lens has in various types of configurations, the common ones being positive achromats, negative achromats, triplet achromats, and aspheric achromats.
Note that an achromatic lens can be a doublet lens(two elements) or triplet (three elements), and the number of elements is independent of the number of rays corrected by the lens.
In other words, an achromatic lens in a doublet or triplet configuration can correct both red and blue light in the visible range.
Because achromatic lenses focus the colors at the same point, they allow the user to fully focus the image. Compared with uncorrected singlet lens, achromatic lens can produce clearer image, which is easier to observe and obtain more accurate perception.
Achromatic lenses revolutionized imaging when they were first introduced, and while the quality of lenses has continued to improve, achromatic lenses remain a staple in both scientific and non-scientific optical applications.
Improved image quality: Achromatic lenses eliminate color banding, greatly improving image brightness and clarity, a fact that is especially true for polychromatic imaging.
Efficient light transmission: Unlike singlet lenses, the on-axis performance of achromatic lenses does not degrade with aperture size, allowing you to utilize the entire transparent aperture.
Cost-effective production: Although achromatic lenses can be improved, these lenses are much more expensive, and for most purposes, achromatic lenses provide a lot of correction, making them the most cost-effective way to obtain clear white light images.
To produce the desired color correction, achromatic lens manufacturers must use two or more types of optical glass, which have different amounts of wave dispersion.
Typically, the process involves concave lens elements with high dispersion and convex lens elements with low dispersion. The two lenses are mounted so that the deformation of one lens closely cancels the deformation of the other lens.
This type of achromatic lens is called an achromatic doublet lens and is the most common type of achromatic lens, although triplets also exist.
Definition: optical devices or setups with minimized chromatic aberrations
Category: general optics
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For purchasing achromatic optics, use the RP Photonics Buyer's Guide – an expert-curated directory for finding all relevant suppliers, which also offers advanced purchasing assistance.Achromatic optics are optical devices or setups which have been optimized such that chromatic aberrations are minimized, such that they can be used in a wide range of wavelengths. Most frequently, this refers to optical lenses or objectives, which are essentially combinations of several lenses. Achromatic optical lenses are often just called achromats. The property of being achromatic (essentially insensitive to wavelength changes) is called achromatism. Achromatic optics, in particular doublet and triplet achromatic lenses, have been invented and used already in the eighteenth century, and are very widely used in modern optical technology.
As the article on chromatic aberrations explains, frequently used parameters are based on refractive index values at certain reference wavelengths. From these, one calculates Abbe numbers such as ($V_\textrm{D}$) or ($V_\textrm{d}$), which then appear in various formulas for calculating the strength of chromatic aberrations. Such equations allow one to calculate parameter combinations (e.g., concerning used materials, curvature radii and spacings between optical elements) for which the axial and/or transverse chromatic aberrations vanish, typically at two or three different wavelengths.
As an example, we consider chromatic aberrations of a lens. A first simple version is an ordinary (non-achromatic) biconvex singlet lens made from BK7 glass, with curvature radii of 103 mm on both surfaces. The substantial chromatic aberrations of that lens are seen in the following diagram, where it has been assumed that a collimated laser beam with an initial beam radius of 1 mm hits that lens. Obviously, the focus position has a substantial wavelength dependence.
(Note that the use of a biconvex lens for focusing a collimated beam is not ideal in terms of spherical aberrations, but this aspect is not relevant for the current discussion.)
For improving the situation, we can now use an achromatic lens doublet, consisting two parts (see Figure 2): a biconvex lens made of BK7 and concave-convex lens made of SF2 (a flint glass). The basic idea is to realize an overall focusing lens by combining a strongly focusing and a less strongly defocusing lens, where the latter exhibits stronger chromatic dispersion. Although the defocusing effect of the second lens is weaker than the focusing effect on the first one, its chromatic aberrations can compensate those of the other lens.
The considered doublet lens design has been numerically optimized with the RP Resonator software such that we obtain a focal length close to 100 mm (measured from the middle of the lens at ($z$) = 2 mm) in the wavelength range from 400 nm to 800 nm. The curvature radius on the left side has been fixed at 60 mm, and the other two curvature radii were subject to optimization. The inner radii of curvature of the two lenses are required to be the same, so that the two lenses can be contacted (e.g. cemented together), forming a single optical element and minimizing reflection losses. Note that for the given focal length the double lens requires a stronger curvature due to the defocusing effect of the flint lens.
Figure 3 shows the resulting foci; one can see that the focus positions agree quite well for three very different wavelengths.
Figure 4 shows the residual wavelength dependence of the focal length. One can see that the chromatic compensation is good but not perfect.
Other doublet lens designs are flat on one side (plano-concave designs), and one can also realize defocusing achromatic lenses (negative achromats). In some cases, a lens doublet is not contacted, but the two lenses are only placed in a common housing (air-spaced doublets). Furthermore, there are cylindrical lenses designed as achromats.
With such a doublet lens design, one can adjust the parameters such that the axial chromatic aberrations exactly vanish for two wavelengths (typically in the red and blue spectral region). By combining three different materials (making aspheric triplets), it is possible to make a so-called apochromatic lens (apochromat), where the chromatic aberrations vanish for three different wavelengths. Although in principle the distortions at other wavelengths are not limited by such conditions, they are typically smaller for an apochromat at least within a certain wavelength range.
In the same way as other lenses, achromats can be optimized for additional requirements such as minimizing spherical aberrations and coma in certain situations, and can be equipped with sufficiently broadband anti-reflection coatings. Also, there are mounted and unmounted achromats.
Particularly high performance in terms of the magnitude of remaining chromatic aberrations can be achieved with superachromatic lens designs, involving fluoride glasses and requiring particularly tight fabrication tolerances.
There are also other types of achromatic lenses, which are based on diffractive optics. Here, the operation principle is entirely different from that of the lens doublets as explained above.
Optical prisms are often exactly used for obtaining a wavelength-dependent deflection angle for the light beam, i.e., to exploit chromatic behavior. In some cases, however, it is desirable to obtain a certain deflection angle which is about the same for a wide range of wavelengths. Such a performance can be achieved with essentially the same basic approach as for an achromatic lens doublet: one can combine two prisms made from different optical materials, which may be contacted to obtain a single prism.
It is also possible to design composite prisms such that the average deflection angle in some wavelength range is about zero, but a substantial wavelength dependence of that angle is achieved. That is of course not an achromatic design.
There are also achromatic waveplates, but in this context a different kind of chromatic distortion is reduced: the wavelength dependence of the optical retardance, i.e., of the difference of the optical phase changes caused for two orthogonal polarization directions. Such devices can be made by combining materials with different chromatic dispersion (e.g. quartz and MgF2), which can have a nearly constant retardance over a very wide spectral range (hundreds of nanometers).
The main application of achromatic optics (in particular, on a chromatic lenses) is in imaging systems, as needed for photography, microscopy and video recording, for example, as those applications typically involve a broad wavelength range. In many cases, it is not sufficient to use a simple doublet lens; instead, one requires a more complex objective, containing multiple lenses. The typical approach for compensating the chromatic aberrations of such a system is not to build it from achromats only, but rather to find an optical design where only the overall chromatic aberrations are more or less compensated. Of course, chromatic aberrations are typically only one of several types of optical aberrations which need to be minimized, and additional requirements such as a compact design or highlight throughput can make it even more difficult to find a good compromise between all requirements.
Achromatic optics are not only required in the visible spectral region, but also for infrared and ultraviolet light. Particularly strong dispersion is to be compensated in the ultraviolet spectral region, but there are also applications in the infrared where two or more very different wavelengths or a very wide range of wavelengths are involved. For example, achromats are beneficial for focusing or collimating the output of supercontinuum sources or in other cases with ultrabroadband ultrashort pulses.
In some applications, it is possible to avoid any chromatic aberrations by using reflective optics instead of lenses. Curved mirrors, which can be used for focusing a beam, for example, are naturally achromatic; this applies even to dielectric mirrors, despite the wavelength dependence of the used multilayer materials.
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