A microlens is a small lens, generally with a diameter less than a millimetre (mm) and often as small as 10 micrometres (µm). The small sizes of the lenses means that a simple design can give good optical quality but sometimes unwanted effects arise due to optical diffraction at the small features. A typical microlens may be a single element with one plane surface and one spherical convex surface to refract the light. Because microlenses are so small, the substrate that supports them is usually thicker than the lens and this has to be taken into account in the design. More sophisticated lenses may use aspherical surfaces and others may use several layers of optical material to achieve their design performance.
A different type of microlens has two flat and parallel surfaces and the focusing action is obtained by a variation of refractive index across the lens. These are known as gradient-index (GRIN) lenses. Some microlenses achieve their focusing action by both a variation in refractive index and by the surface shape.
Another class of microlens, sometimes known as micro-Fresnel lenses, focus light by refraction in a set of concentric curved surfaces. Such lenses can be made very thin and lightweight. Binary-optic microlenses focus light by diffraction. They have grooves with stepped edges or multilevels that approximate the ideal shape. They have advantages in fabrication and replication by using standard semiconductor processes such as photolithography and RIE.
Microlens arrays contain multiple lenses formed in a one-dimensional or two-dimensional array on a supporting substrate. If the individual lenses have circular apertures and are not allowed to overlap they may be placed in a hexagonal array to obtain maximum coverage of the substrate. However there will still be gaps between the lenses which can only be reduced by making the microlenses with non-circular apertures. With optical sensor arrays tiny lens systems serve to focus and concentrate the light onto the photodiode surface instead of allowing it to fall on non-photosensitive areas of the pixel device. Fill-factor is the ratio of the active refracting area, i.e. that area which directs light to the photosensor, to the total contiguous area occupied by the microlens array.
In the 17th century, Robert Hooke and Antonie van Leeuwenhoek both developed techniques to make small glass lenses for use with their microscopes. Hooke melted small filaments of Venetian glass and allowed the surface tension in the molten glass to form the smooth spherical surfaces required for lenses, then mounting and grinding the lenses using conventional methods. The principle has been repeated by performing photolithography into materials such as photoresist or UV curable epoxy and melting the polymer to form arrays of multiple lenses. More recently microlens arrays have been fabricated using convective assembly of colloidal particles from suspension.
Advances in technology have enabled microlenses to be designed and fabricated to close tolerances by a variety of methods. In most cases multiple copies are required and these can be formed by moulding or embossing from a master lens array. The master lens array may also be replicated through the generation of an electroform using the master lens array as a mandrel. The ability to fabricate arrays containing thousands or millions of precisely spaced lenses has led to an increased number of applications.
The optical efficiency of diffracting lenses depends on the shape of the groove structure and, if the ideal shape can be approximated by a series of steps or multilevels, the structures may be fabricated using technology developed for the integrated circuit industry, such as wafer-level optics. This area[clarification needed] is known as binary optics.
Microlenses in recent imaging chips have attained smaller and smaller sizes. The Canon EOS-1Ds Mark III packs 21.1 million microlenses onto its CMOS imaging chip, one per photosite, each just 6.4 micrometer across. An announced Sony DSLR 24.6MP image sensor will have even smaller microlenses.
Microlenses can be also made from liquids.
Wafer-level optics 
Wafer-level optics (WLO) enables the design and manufacture of miniaturized optics at the wafer level using advanced semiconductor-like techniques. The end product is cost effective, miniaturized optics that enable the reduced form factor of camera modules for mobile devices.
The technology is scalable from a single-element CIF/VGA lens to a multi-element mega pixel lens structure, where the lens wafers are precision aligned, bonded together and diced to form multi-element lens stacks. As of 2009 the technology was used in about 10 percent of the mobile phone camera lens market.
Single microlenses are used to couple light to optical fibres while microlens arrays are often used to increase the light collection efficiency of CCD arrays. They collect and focus light that would have otherwise fallen on to the non-sensitive areas of the CCD. Microlens arrays are also used in some digital projectors, to focus light to the active areas of the LCD used to generate the image to be projected. Current research also relies on microlenses of various types to act as concentrators for high efficiency photovoltaics for electricity production.
Combinations of microlens arrays have been designed that have novel imaging properties, such as the ability to form an image at unit magnification and not inverted as is the case with conventional lenses. Microlens arrays have been developed to form compact imaging devices for applications such as photocopiers and mobile-phone cameras.
Another application is in 3D imaging and displays. In 1902 Frederic E. Ives proposed the use of an array of alternately transmitting and opaque strips to define the viewing directions for a pair of interlaced images and hence enable the observer to see a 3D stereoscopic image. The strips were later replaced by Hess with an array of cylindrical lenses known as a lenticular screen, to make more efficient use of the illumination.
Hitachi have 3D displays free of 3D glasses using arrays of microlens to create the stereoscopic pictures felling.
More recently, the availability of arrays of spherical microlenses has enabled Gabriel Lippmann’s idea for integral photography to be explored and demonstrated. Colloidal microlenses have also enabled single molecule detection when used in conjunction with a long working distance, low light collection efficiency objective lens.
Microlens Arrays are also used by Lytro to achieve Light Field Photography (Plenoptic Camera) that eliminates the need for initial focusing prior to capturing images. Instead, focus is achieved in software during post-processing.
In order to characterise microlenses it is necessary to measure parameters such as the focal length and quality of transmitted wavefront. Special techniques and new definitions have been developed for this.
For example, because it is not practical to locate the principal planes of such small lenses, measurements are often made with respect to the lens or substrate surface. Where a lens is used to couple light into an optical fibre the focused wavefront may exhibit spherical aberration and light from different regions of the microlens aperture may be focused to different points on the optical axis. It is useful to know the distance at which the maximum amount of light is concentrated in the fibre aperture and these factors have led to new definitions for focal length. To enable measurements on microlenses to be compared and parts to be interchanged, a series of international standards has been developed to assist users and manufacturers by defining microlens properties and describing appropriate measurement methods.
Microoptics in nature 
Examples of microoptics are to be found in nature ranging from simple structures to gather light for photosynthesis in leaves to compound eyes in insects. As methods of forming microlenses and detector arrays are further developed then the ability to mimic optical designs found in nature will lead to new compact optical systems.
See also 
- Hooke R, Preface to Micrographia. The Royal Society of London. (1665).
- Popovic CD, Sprague RA, Neville Connell GA, "Techniques for monolithic fabrication of microlens arrays", Appl. Opt. 27 1281–1284, (1988).
- Daly D, Stevens R F, Hutley M C, Davies N, "The manufacture of microlenses by melting photoresist". Proceedings of seminar "Microlens Arrays", May 1991. IOP Short Meeting Series No 30, 23–34.
- Kumnorkaew P, Ee Y, Tansu N, and Gilchrist J F, "Investigation of the Deposition of Microsphere Monolayers for Fabrication of Microlens Arrays", Langmuir, 24, 12150-12157, (2008)
- Borrelli, N F. Microoptics technology: fabrication and applications of lens arrays and devices. Marcel Dekker, New York (1999).
- Veldkamp W B, McHugh T J. "Binary optics", Scientific American, Vol. 266 No. 5 pp 50–55, (May 1992).
- S. Grilli; L. Miccio, V. Vespini, A. Finizio, S. De Nicola, and P. Ferraro (2008). "Liquid micro-lens array activated by selective electrowetting on lithium niobate substrates". Optics Express 16 (11): 8084–8093. doi:10.1364/OE.16.008084. PMID 18545521.
- "Wafer-Level Camera Technologies Shrink Camera Phone Handsets", Photonics.com, August 2007.
- J. H. Karp; E. J. Tremblay and J. E. Ford (2010). "Planar micro-optic solar concentrator". Optics Express 18 (2): 1122–1133. doi:10.1364/OE.18.001122. PMID 20173935.
- Ives FE. Parallax stereogram and process of making same. US Patent 725,567 (1903).
- Hess W. Improved manufacture of stereoscopic pictures. UK Patent 13,034 (1912).
- Lippmann G. "Epreuves reversibles. Photographies integrales", Comptes Rendus 146 446–451 (1908).
- Stevens R F, Davies N. "Lens arrays and photography". The Journal of Photographic Science. Vol 39 pp 199–208, (1991).
- Schwartz JJ; Stavrakis S and Quake SR (2010). "Colloidal lenses allow high-temperature single-molecule imaging and improve fluorophore photostability". Nature Nanotechnology 5: 127–132. doi:10.1038/nnano.2009.452. PMID 20023643.
- Iga K, Kokburn Y, Oikawa M. Fundamentals of microoptics. Academic Press, London (1984).
- ISO 14880-1:2001. Optics and photonics - Microlens arrays - Part 1: Vocabulary
- ISO 14880-2:2006. Optics and photonics - Microlens arrays - Part 2: Test methods for wavefront aberrations
- ISO 14880-3:2006. Optics and photonics - Microlens arrays - Part 3: Test methods for optical properties other than wavefront aberrations
- ISO 14880-4:2006. Optics and photonics - Microlens arrays - Part 4: Test methods for geometrical properties.
- Land M. "The optics of animal eyes". Proc Royal Institution, vol 57, pp. 167–189, (1985)
- Duparré J. et al., "Microoptical telescope compound eye". Optics Express, Vol. 13, Issue 3, pp. 889–903 (2005).