Anti-Reflection (AR) coatings are functional dielectric thin films deposited on the surface of optical components. Serving as a fundamental and indispensable optical technology, they are designed to reduce interfacial reflection, boost optical transmittance, and suppress stray light and ghost images. These coatings have become a standard process in modern optical systems, widely applied in consumer, industrial and scientific optoelectronic devices.
The fundamental working principle of AR coatings is destructive light interference. In natural conditions, when light travels from air (refractive index n₀≈1.0) to common glass substrates (refractive index nₛ≈1.5), Fresnel reflection occurs at the interface, causing a single-side reflectivity of approximately 4%. For multi-lens optical systems, the superposition of continuous reflection loss drastically reduces overall light transmittance and degrades imaging quality. To eliminate this issue, most AR coatings adopt a quarter-wavelength (λ/4) structural design that meets two core conditions for complete light cancellation.
The first is the phase condition: the physical thickness of the coating is precisely one-quarter of the target working wavelength, generating a 180° phase difference between the reflected light from the top coating surface and the bottom substrate-coating interface. The second is the amplitude condition: the refractive index of the coating material satisfies the formula $$n_1=\sqrt{n_0 \times n_s}$$, enabling the two reflected light waves to have equal amplitude and offset each other completely, thereby minimizing surface reflection to the greatest extent.
Based on structural design, material combination and performance characteristics, AR coatings are classified into three mainstream types: single-layer AR coatings, multi-layer AR coatings and special gradient-index AR structures. Single-layer AR coatings are typically fabricated with single low-refractive-index materials, predominantly magnesium fluoride (MgF₂), with a standard λ/4 optical thickness. This structure features a simple fabrication process, low cost and high maturity. However, it only delivers optimal anti-reflection effects within a narrow spectral range. At the visible central wavelength of 550 nm, its minimum reflectivity is no more than 1.5%. It is mainly used for low-end optical products such as ordinary spectacle lenses and basic optical windows.
Multi-layer AR coatings consist of 3 to 10 alternating stacks of high and low refractive index dielectric materials, with silicon dioxide (SiO₂) and tantalum pentoxide (Ta₂O₅) being the most common combinations. Different from narrowband single-layer coatings, multi-layer structures achieve broadband anti-reflection performance covering visible and near-infrared bands, with the optimal reflectivity reduced to below 0.5% in the target spectral range. Meanwhile, they possess excellent angular stability under standard incident angles (0°–45°) and can adapt to wider incident angles up to 60° for customized designs. Owing to their superior performance, multi-layer AR coatings are the dominant choice for high-precision optical equipment, including smartphone camera modules, SLR lenses, telescopes and professional laser optical systems.
Special advanced AR structures mainly include moth-eye bionic microstructures and continuous gradient-index coatings. The moth-eye structure is a typical bionic optical design with gradual refractive index changes on the substrate surface. It achieves ultra-broadband and ultra-low reflection performance without traditional layered film interfaces. Similarly, gradient-index AR coatings feature continuously varying refractive index from the air-film interface to the substrate, completely eliminating abrupt refractive index changes and interface reflection. These novel structures are widely adopted in high-end display screens and photovoltaic solar cell systems due to their outstanding wide-spectrum and wide-angle anti-reflection capabilities.
The performance of AR coatings is evaluated by a series of core technical parameters. The key indicators cover working spectral bands, including ultraviolet (UV), visible (VIS), near-infrared (NIR) and infrared (IR) regions. The standard reflectivity threshold is defined as R<1.5% for single-layer coatings and R<0.5% for multi-layer coatings in the target band. The conventional acceptable angle of incidence (AOI) ranges from 0° to 45°, while high-performance wide-angle coatings support up to 60°. In addition, environmental stability, including temperature resistance, moisture resistance and wear resistance (enhanced by DLC hard coatings), is a critical indicator for industrial application.
AR coating materials are strictly selected according to their refractive index characteristics. Low-refractive-index materials (n=1.3–1.5) mainly include MgF₂, SiO₂ and Al₂O₃, which serve as spacer layers in multi-layer structures. High-refractive-index materials (n=2.0–2.5) primarily contain TiO₂, Ta₂O₅, ZrO₂ and Nb₂O₅, which cooperate with low-index materials to form interference cycles. For ultraviolet optical systems, special low-absorption materials such as LaF₃ and YF₃ are applied to avoid light loss and film aging under UV irradiation.
Three mainstream fabrication techniques are widely used for AR coating manufacturing. Physical Vapor Deposition (PVD), represented by electron beam evaporation and magnetron sputtering, is the dominant industrial process. It produces coatings with high uniformity and stable performance, suitable for large-scale mass production. Atomic Layer Deposition (ALD) enables precise atomic-level thickness control and superior conformal coverage, making it ideal for coating complex curved surfaces and micro-nano structures with high precision. The sol-gel method is a low-cost, large-area coating technology, which is economical and applicable for glass and plastic substrate coating in civilian optical products.
Benefiting from diversified structural designs and mature manufacturing processes, AR coatings are applied in multiple key fields. In consumer optics, they reduce surface glare of spectacle lenses and eliminate ghost images of mobile phone and camera lenses to improve imaging contrast. In precision instruments such as microscopes and spectrometers, they suppress stray light to enhance weak signal detection capability. In laser systems, AR coatings are coated on laser windows, lenses and prisms to reduce back-reflection, protect laser sources and improve system operational stability. In photovoltaic and display industries, they improve the photoelectric conversion efficiency of solar cells and reduce ambient light reflection on display screens and touch panels. Moreover, they are widely used in security monitoring lenses and vehicle-mounted HUD devices to optimize imaging clarity and reduce glare interference.
In summary, AR coatings solve the inherent interfacial reflection problem of optical elements based on destructive interference theory. With technical iterations from low-cost single-layer structures to high-performance multi-layer and bionic gradient structures, they cover full spectral bands from ultraviolet to infrared. As a core optical technology that improves light utilization efficiency, optimizes imaging quality and enhances system stability, AR coatings will continue to support the innovative development of consumer optics, industrial precision equipment, scientific research optics and new energy industries.