Physics:Phased-array optics
Phased-array optics is the technology of controlling the phase and amplitude of light waves transmitting, reflecting, or captured (received) by a two-dimensional surface using adjustable surface elements. An optical phased array (OPA) is the optical analog of a radio-wave phased array.[1] By dynamically controlling the optical properties of a surface on a microscopic scale, it is possible to steer the direction of light beams (in an OPA transmitter[2]), or the view direction of sensors (in an OPA receiver[3]), without any moving parts. Phased-array beam steering is used for optical switching and multiplexing in optoelectronic devices and for aiming laser beams on a macroscopic scale.
Complicated patterns of phase variation can be used to produce diffractive optical elements, such as dynamic virtual lenses, for beam focusing or splitting in addition to aiming. Dynamic phase variation can also produce real-time holograms. Devices permitting detailed addressable phase control over two dimensions are a type of spatial light modulator (SLM).
Transmitter
An optical phased-array transmitter includes a light source (laser), power splitters, phase shifters, and an array of radiating elements.[4][5][6] The output light of the laser source is split into several branches using a power splitter tree. Each branch is then fed to a tunable phase shifter. The phase-shifted light is input to a radiating element (a nanophotonic antenna) that couples the light into free space. Light radiated by the elements is combined in the far-field and forms the far-field pattern of the array. By adjusting the relative phase shift between the elements, a beam can be formed and steered.
Receiver
In an optical phased-array receiver,[3] the incident light (usually coherent light) on a surface is captured by a collection of nanophotonic antennas that are placed on a 1D[7] or 2D[3] array. The light received by each element is phase-shifted and amplitude-weighted on a chip. These signals are then added together in the optic or electronic domain to form a reception beam. By adjusting the phase shifts, the reception beam can be steered to different directions, and light incident from each direction is collected selectively.
Applications
In nanotechnology, phased-array optics refers to arrays of lasers or SLMs with addressable phase and amplitude elements smaller than a wavelength of light.[8] While still theoretical, such high-resolution arrays would permit extremely realistic three-dimensional image display by dynamic holography with no unwanted orders of diffraction. Applications for weapons, space communications, and invisibility by optical camouflage have also been suggested.[8]
DARPA's Excalibur program aims to provide realtime correction of atmospheric turbulence for a laser weapon.[9]
See also
References
- ↑ McManamon P. F. (May 15, 1996). "Optical phased array technology". Proceedings of the IEEE, Laser Radar Applications (IEEE) 84 (2): 99–320. http://cat.inist.fr/?aModele=afficheN&cpsidt=3024704. Retrieved 2007-02-18.
- ↑ Sun J. (January 1, 2013). "Large-scale nanophotonic phased array". Nature (Nature Publishing Group, a division of Macmillan Publishers Limited) 493 (195): 195–199. doi:10.1038/nature11727. PMID 23302859. Bibcode: 2013Natur.493..195S.
- ↑ 3.0 3.1 3.2 Fatemi R. (Nov 12, 2018). "High sensitivity active flat optics optical phased array receiver with a two-dimensional aperture". Opt. Express (Optical Society of America) 26 (23): 29983–29999. doi:10.1364/OE.26.029983. PMID 30469879. Bibcode: 2018OExpr..2629983F. https://authors.library.caltech.edu/91516/1/oe-26-23-29983.pdf.
- ↑ Poulton C. (2017). "Large-scale silicon nitride nanophotonic phased arrays at infrared and visible wavelengths". Opt. Lett. (Optical Society of America) 42 (1): 21–24. doi:10.1364/OL.42.000021. PMID 28059212. Bibcode: 2017OptL...42...21P.
- ↑ Chung S. (Jan 2018). "A Monolithically Integrated Large-Scale Optical Phased Array in Silicon-on-Insulator CMOS". IEEE Journal of Solid-State Circuits (IEEE) 53 (1): 275–296. doi:10.1109/JSSC.2017.2757009. Bibcode: 2018IJSSC..53..275C.
- ↑ Aflatouni F. (August 4, 2015). "Nanophotonic projection system". Opt. Express (Optical Society of America) 23 (16): 21012–21022. doi:10.1364/OE.23.021012. PMID 26367953. Bibcode: 2015OExpr..2321012A.
- ↑ Fatemi R. (2016). "A One-Dimensional Heterodyne Lens-Free OPA Camera". Conference on Lasers and Electro-Optics, OSA Technical Digest (2016). Optical Society of America. pp. STu3G.3. http://www.osapublishing.org/abstract.cfm?URI=CLEO_SI-2016-STu3G.3. Retrieved 13 February 2019.
- ↑ 8.0 8.1 Wowk B. (1996). "Phased Array Optics". in B. C. Crandall. Molecular Speculations on Global Abundance. MIT Press. pp. 147–160. ISBN 0-262-03237-6. http://www.phased-array.com/1996-Book-Chapter.html. Retrieved 2007-02-18.
- ↑ Eshel, Tamir (7 March 2014). "Successful EXCALIBUR Test Brings DARPA Closer to Compact High Energy Lasers". Defense Update. http://defense-update.com/20140307_successful-excalibur-test-brings-darpa-closer-compact-high-energy-lasers.html. Retrieved 9 March 2014.
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