Extreme-depth-of-focus imaging with a flat lens

被引:100
作者
Banerji, Sourangsu [1 ]
Meem, Monjurul [1 ]
Majumder, Apratim [1 ]
Sensale-Rodriguez, Berardi [1 ]
Menon, Rajesh [1 ,2 ]
机构
[1] Univ Utah, Dept Elect & Comp Engn, Salt Lake City, UT 84102 USA
[2] Oblate Opt Inc, San Diego, CA 92130 USA
基金
美国国家科学基金会;
关键词
EXTENDED DEPTH; FOCAL DEPTH; LIGHT;
D O I
10.1364/OPTICA.384164
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
A lens performs an approximately one-to-one mapping from the object to the image plane. This mapping in the image plane is maintained within a depth of field (or referred to as depth of focus, if the object is at infinity). This necessitates refocusing of the lens when the images are separated by distances larger than the depth of field. Such refocusing mechanisms can increase the cost, complexity, and weight of imaging systems. Here we show that by judicious design of a multi-level diffractive lens (MDL) it is possible to drastically enhance the depth of focus by over 4 orders of magnitude. Using such a lens, we are able to maintain focus for objects that are separated by as large a distance as similar to 6m in our experiments. Specifically, when illuminated by collimated light at lambda = 0.85 mu m, the MDL produced a beam, which remained in focus from 5 to 1200 mm. The measured full width at half-maximum of the focused beam varied from 6.6 mu m(5 mm away from the MDL) to 524 mu m (1200 mm away from the MDL). Since the side lobes were well suppressed and the main lobe was close to the diffraction limit, imaging with a horizontal x vertical field of view of 40 degrees x 30 degrees over the entire focal range was possible. This demonstration opens up a new direction for lens design, where by treating the phase in the focal plane as a free parameter, extreme-depth-of-focus imaging becomes possible. (C) 2020 Optical Society of America under the terms of the OSA Open Access Publishing Agreement
引用
收藏
页码:214 / 217
页数:4
相关论文
共 25 条
[1]  
Banerji S., 2019, ARXIV190706251PHYSIC
[2]   Ultra-thin near infrared camera enabled by a flat multi-level diffractive lens [J].
Banerji, Sourangsu ;
Meem, Monjurul ;
Majumder, Apratim ;
Guevara, Fernando Vasquez ;
Sensale-Rodriguez, Berardi ;
Menon, Rajesh .
OPTICS LETTERS, 2019, 44 (22) :5450-5452
[3]   Single flat lens enabling imaging in the short-wave infra-red (SWIR) band [J].
Banerji, Sourangsu ;
Meem, Monjurul ;
Majumder, Apratim ;
Dvonch, Curt ;
Sensale-Rodriguez, Berardi ;
Menon, Rajesh .
OSA CONTINUUM, 2019, 2 (10) :2968-2974
[4]   3D-printed diffractive terahertz optical elements through computational design [J].
Banerji, Sourangsu ;
Sensale-Rodriguez, Berardi .
MICRO- AND NANOTECHNOLOGY SENSORS, SYSTEMS, AND APPLICATIONS XI, 2019, 10982
[5]   Imaging with flat optics: metalenses or diffractive lenses? [J].
Banerji, Sourangsu ;
Meem, Monjurul ;
Majumder, Apratim ;
Vasquez, Fernando Guevara ;
Sensale-Rodriguez, Berardi ;
Menon, Rajesh .
OPTICA, 2019, 6 (06) :805-810
[6]   A Computational Design Framework for Efficient, Fabrication Error-Tolerant, Planar THz Diffractive Optical Elements [J].
Banerji, Sourangsu ;
Sensale-Rodriguez, Berardi .
SCIENTIFIC REPORTS, 2019, 9 (1)
[7]  
Born M., 1999, Principle of Optics
[8]   New paradigm for imaging systems [J].
Cathey, WT ;
Dowski, ER .
APPLIED OPTICS, 2002, 41 (29) :6080-6092
[9]   Electronic imaging using a logarithmic asphere [J].
Chi, WL ;
George, N .
OPTICS LETTERS, 2001, 26 (12) :875-877
[10]   EXTENDED DEPTH OF FIELD THROUGH WAVE-FRONT CODING [J].
DOWSKI, ER ;
CATHEY, WT .
APPLIED OPTICS, 1995, 34 (11) :1859-1866