Toggle menu
Toggle preferences menu
Toggle personal menu
Not logged in
Your IP address will be publicly visible if you make any edits.

Catadioptric system

vrarwiki.com · VR & AR Wiki

A catadioptric system is an optical system that uses both refraction and reflection, usually by combining lenses with curved mirrors. The name joins two older terms of optics: dioptrics, the study of refracting elements (lenses), and catoptrics, the study of reflecting surfaces (mirrors).[1] Catadioptric designs appear in lighthouse lenses, astronomical telescopes, long camera lenses and wide-angle cameras. Designers use them to correct aberrations and to fit a long optical path into a short package.[2]

In virtual reality (VR) headsets, the polarization-based folded lens usually called a pancake lens is a catadioptric system. A 2024 paper by researchers at the University of Central Florida describes this "polarization-based folded optics, often referred to as catadioptric or pancake optics" as the design used in compact headsets such as the Apple Vision Pro and Meta Quest Pro.[3] In augmented reality (AR), researchers have described catadioptric versions of the birdbath combiner for see-through near-eye displays.[4] In imaging, catadioptric cameras that pair a conventional camera with a curved mirror capture very wide fields of view, a property that computer vision researchers have linked to applications including model acquisition for virtual reality.[1]

Reviewed 19 October 2026. Every claim checked against the opened sources: Baker and Nayar 1999, Ding et al. 2024 and Li et al. 2021 full text, Xiong et al. 2021, the Nayar 1997, Li et al. 2024, Geyer and Daniilidis 2000, Gurrieri and Dubois 2013 and MirrorNeRF abstracts, Terebizh 2007, JBAA 2004, Hamburg Observatory, Nikon, USLHS, NPS, Cordouan and RP Photonics pages, with paper metadata confirmed via Crossref. About review dates.

Definition

A purely refracting (dioptric) system forms an image with lenses alone, and a purely reflecting (catoptric) system uses only mirrors. A catadioptric system uses both. In their 1999 analysis of catadioptric cameras, Simon Baker and Shree K. Nayar define catadioptric image formation as "the approach of using mirrors in combination with conventional imaging systems" and note that the combination of refracting and reflecting elements is referred to as catadioptrics.[1] The RP Photonics Encyclopedia describes catadioptric telescopes as designs that "combine refractive and reflective optical elements to correct aberrations and compact the system".[2]

Reflection and refraction can also happen inside one glass element. Fresnel's lighthouse lenses work by refraction at glass surfaces, and the French national monument site for the Cordouan lighthouse explains that "total reflection" (total internal reflection inside the glass) is used in the so-called catadioptric parts of the apparatus.[5] A Mangin mirror is a spherical meniscus lens whose back surface is made reflective, so light passes through the glass, reflects, and passes through it again.[6]

The mix of elements gives designers more variables. A reflecting surface adds optical power without adding chromatic aberration, while a corrector plate can compensate for the spherical aberration of a spherical mirror.[7][8] Folding the light path back on itself with mirrors also shortens the physical length of the system.[2]

History

Lighthouse lenses and the Mangin mirror

The United States Lighthouse Society's chronology of Fresnel lens development lists "Fresnel's First Catadioptric Lens" in 1826, three years after Augustin Fresnel's first first-order flashing lens was installed at Cordouan in France. It credits Alan Stevenson with the first use of lower prisms ("Lower Catadioptric Panels") in a flashing lens, the 1840 Skerryvore lens in Scotland.[9] The U.S. National Park Service records that a rotating, catadioptric, third-order Fresnel lens was installed in the Anacapa Island lighthouse in California in 1932.[10]

The back-silvered spherical meniscus, or Mangin mirror, also predates modern catadioptric telescopes. Astronomer V. Yu. Terebizh writes that it has been applied in astronomy since early work by W. F. Hamilton (an 1814 English patent), Mangin (1876) and Schuppmann (1899).[6]

Telescopes

The Estonian-born optician Bernhard Schmidt, who worked at the Hamburg Observatory in Bergedorf, designed a wide-field astronomical camera that pairs a spherical main mirror with a corrector plate. The corrector counteracts the spherical aberration of the mirror away from the optical axis.[8] According to a history of the observatory in the Journal of the British Astronomical Association, the first Schmidt corrector plate was built in the winter of 1929, and the first Schmidt telescope was completed in 1930.[11] The observatory lists that first instrument with a mirror diameter of 44 cm, an aperture of 36 cm and a focal length of 62.5 cm.[8]

D. D. Maksutov, of the State Optical Institute in Moscow, published "New Catadioptric Meniscus Systems" in the Journal of the Optical Society of America in May 1944.[12] The RP Photonics Encyclopedia names the Schmidt-Cassegrain and Maksutov-Cassegrain telescopes as well-known examples of catadioptric telescopes.[2]

Mirror lenses for cameras

Reflex lenses for cameras apply the same combination of mirrors and lenses to long focal lengths. Nikon's official lens history says long refractive lenses grow bulky and become harder to correct for chromatic aberration as focal length increases, and that reflex lenses "applied the effect of reflection of a mirror to solve the two problems". In the construction Nikon describes, light passes through a front lens, reflects from an annular concave main mirror onto a convex secondary mirror formed on part of that front lens, and then passes through a refractive lens group set in a hole in the main mirror to form the image. Nikon dates its first reflex lens for cameras to 1960 and released the Reflex-Nikkor 500mm f/8 in 1969; the revised version of April 1984 weighs 840 g and focuses down to 1.5 m. Because the secondary mirror blocks the center of the aperture, out-of-focus highlights from such lenses take an annular (ring) shape.[13]

Catadioptric cameras and omnidirectional imaging

Conventional cameras see only a narrow cone of directions. Placing a curved mirror in front of a camera lets one sensor capture a much wider field, which Baker and Nayar list as useful for surveillance, teleconferencing, model acquisition for virtual reality, ego-motion estimation and tracking.[1]

Baker and Nayar note that it is highly desirable for the whole system to have a single effective viewpoint (center of projection). With one viewpoint, every pixel measures light arriving along a known direction through that point, so software can map the image into geometrically correct perspective images.[1] In a 1997 paper at the IEEE Conference on Computer Vision and Pattern Recognition, Shree K. Nayar presented a catadioptric camera with a hemispherical field of view that meets this constraint. He noted that two such cameras placed back to back give a fully omnidirectional sensor, and showed software generation of perspective images for any user-selected viewing direction and magnification.[14]

In the 1999 paper, Baker and Nayar derived the complete class of single-lens, single-mirror catadioptric sensors with a single viewpoint. The mirror profiles are swept conic sections. A single planar mirror satisfies the constraint but does not enlarge the field of view, and conical and spherical mirrors are degenerate solutions that cannot give a wide field with a single viewpoint (although both have been used in wide-angle sensors without one). Ellipsoidal and hyperboloidal mirrors are realizable solutions, with the camera pinhole and the viewpoint at the two foci. With an orthographic camera, the only solution is a paraboloidal mirror, which simplifies calibration because the mirror can be translated without breaking the constraint. The paper credits Rees (1970) as apparently the first to use a hyperboloidal mirror with a perspective lens for a wide-field, single-viewpoint camera.[1]

Christopher Geyer and Kostas Daniilidis showed in 2000 that all central (single-viewpoint) catadioptric systems are isomorphic to projective mappings from a sphere to a plane, and used this unifying theory to propose a calibration scheme that works from a single view.[15] Luis E. Gurrieri and Eric Dubois published a comparative review in 2013 of cameras and methods for acquiring omnidirectional stereoscopic (panoramic 3D) images and video of dynamic scenes, with possible uses in free-viewpoint 3D television and stereoscopic telepresence; catadioptric cameras are among the paper's listed keywords.[16]

Applications in VR and AR

Pancake lenses

A conventional polarization-based pancake lens has four parts: a half-mirror, a refractive lens, a quarter-wave plate and a reflective polarizer. Light from the display crosses the cavity between the half-mirror and the reflective polarizer three times before it exits, and folding the path this way gives a shorter focal length and a much smaller volume.[17][3] Among their background references for pancake optics, Ding and colleagues cite a 1978 SPIE paper by Joseph A. LaRussa and Arthur T. Gill titled "The Holographic Pancake Window", published in the proceedings volume Visual Simulation and Image Realism I.[3][18]

A 2021 review of AR and VR display optics in Light: Science & Applications explains why the reflective element matters. The curved reflective surface has no chromatic aberration and supplies much of the optical power, so the refractive lenses can be weaker and add less color error; a mirror with positive power also compensates the field curvature of positive refractive lenses. Compared with Fresnel lenses, pancake lenses have smooth surfaces with far fewer diffraction artifacts and less stray light.[7]

The same review identifies low light efficiency as the main drawback. Because light meets the half-mirror twice, the maximum efficiency is 25% for polarized input and 12.5% for unpolarized input. Reflections from the many surfaces and polarization leakage can also create ghost images. As a result, the review says, a catadioptric pancake VR headset usually shows darker images and lower contrast than a comparable dioptric (refractive) headset.[7]

Research on these optics targets those weaknesses:

Year Authors Approach Reported result
2021 Li, Zhan, Yang, Xu, LiKamWa, Li and Wu (University of Central Florida and Goertek Electronics) A broadband cholesteric liquid crystal (CLC) lens, 1 inch in diameter with a 770 mm focal length, replaces the quarter-wave plate and reflective polarizer of a conventional pancake lens Lateral chromatic aberration "suppressed significantly", especially at large field of view; reflection efficiency above 90% across the display spectrum[17]
2024 Ding, Luo, Borjigin and Wu (University of Central Florida and University of Tsukuba) The lossy half-mirror is replaced by a nonreciprocal polarization rotator (a commercial Faraday rotator) placed between two reflective polarizers Measured optical efficiency of 71.5%; the authors estimate that antireflection coatings and better reflective polarizers could raise it to about 93.2%, roughly four times a conventional pancake lens[3]

Birdbath combiners

In AR, a birdbath combiner uses a beam splitter and a half mirror, and the beam splitter folds the optical path. The 2021 Light: Science & Applications review notes that, compared with a single-combiner design, the birdbath adds optics on the display side that give room for aberration correction.[7] Yang Li and colleagues at the Beijing Institute of Technology published a "compact coaxial catadioptric" birdbath design in 2024. It uses a Mangin lens as the reflector and adds polarization elements to address the low energy efficiency of the classic birdbath. The design pairs a 0.71-inch microdisplay with a 50 degree diagonal field of view, an 8 by 6 mm exit pupil diameter, 15.7 mm of eye relief and a maximum total length of 15.4 mm, and the authors fabricated a prototype.[4]

Capture for VR and AR content

Catadioptric imaging has also been applied in research on capturing people for VR and AR. A 2021 arXiv preprint, MirrorNeRF, combined catadioptric imaging (an array of spherical mirrors viewed by a single camera) with neural radiance fields for one-shot portrait reconstruction; its authors state that photorealistic reconstruction of human portraits is critical for many VR and AR applications.[19]

See also

References

  1. ↑ 1.0 1.1 1.2 1.3 1.4 1.5 Simon Baker, Shree K. Nayar (1999-11). "A Theory of Single-Viewpoint Catadioptric Image Formation". International Journal of Computer Vision, vol. 35, no. 2. pp. 175-196. doi:10.1023/A:1008128724364. https://doi.org/10.1023/A:1008128724364. Retrieved 2026-10-19.
  2. ↑ 2.0 2.1 2.2 2.3 Rüdiger Paschotta. "Telescopes". RP Photonics Encyclopedia. RP Photonics AG. doi:10.61835/gf6. https://www.rp-photonics.com/telescopes.html. Retrieved 2026-10-19.
  3. ↑ 3.0 3.1 3.2 3.3 Yuqiang Ding, Zhenyi Luo, Garimagai Borjigin, Shin-Tson Wu (2024). "Breaking the optical efficiency limit of virtual reality with a nonreciprocal polarization rotator". Opto-Electronic Advances, vol. 7, no. 3, article 230178. doi:10.29026/oea.2024.230178. https://doi.org/10.29026/oea.2024.230178. Retrieved 2026-10-19.
  4. ↑ 4.0 4.1 Yang Li, Dewen Cheng, Yilun Huang, Qichao Hou, Yongtian Wang (2024-05). "Design and fabrication of a compact coaxial catadioptric augmented reality near-eye display enabled by genetic algorithm". Optics and Lasers in Engineering, vol. 176, article 108112. doi:10.1016/j.optlaseng.2024.108112. https://doi.org/10.1016/j.optlaseng.2024.108112. Retrieved 2026-10-19.
  5. ↑ "Fresnel's lens". Phare de Cordouan. French Ministry of Culture. https://cordouan.culture.gouv.fr/en/fresnels-lens. Retrieved 2026-10-19.
  6. ↑ 6.0 6.1 V. Yu. Terebizh (2007-10-11). "Wide-field telescopes with a Mangin mirror". arXiv:0710.2165 [astro-ph]. https://arxiv.org/abs/0710.2165. Retrieved 2026-10-19.
  7. ↑ 7.0 7.1 7.2 7.3 Jianghao Xiong, En-Lin Hsiang, Ziqian He, Tao Zhan, Shin-Tson Wu (2021-10-25). "Augmented reality and virtual reality displays: emerging technologies and future perspectives". Light: Science & Applications, vol. 10, article 216. doi:10.1038/s41377-021-00658-8. https://doi.org/10.1038/s41377-021-00658-8. Retrieved 2026-10-19.
  8. ↑ 8.0 8.1 8.2 "Bernhard Schmidt". Hamburg Observatory. Universität Hamburg. https://www.physik.uni-hamburg.de/en/hs/outreach/tour/09-bernhard-schmidt.html. Retrieved 2026-10-19.
  9. ↑ "Fresnel Lens Development Chronology". United States Lighthouse Society. https://uslhs.org/node/1426. Retrieved 2026-10-19.
  10. ↑ "The Fresnel Lens". Channel Islands National Park. National Park Service. https://home.nps.gov/chis/learn/historyculture/fresnellens.htm. Retrieved 2026-10-19.
  11. ↑ Stuart R. Anderson, Dieter Engels (2004). "A short history of Hamburg Observatory". Journal of the British Astronomical Association, vol. 114, no. 2. https://www.physik.uni-hamburg.de/hs/subsite---services/library/_documents/jbaa114.pdf. Retrieved 2026-10-19.
  12. ↑ D. D. Maksutov (1944-05-01). "New Catadioptric Meniscus Systems". Journal of the Optical Society of America, vol. 34, no. 5. pp. 270-284. doi:10.1364/JOSA.34.000270. https://opg.optica.org/josa/abstract.cfm?uri=josa-34-5-270. Retrieved 2026-10-19.
  13. ↑ Haruo Sato. "NIKKOR - The Thousand and One Nights No.13". Nikon Imaging. Nikon Corporation. https://imaging.nikon.com/history/story/0013/index.htm. Retrieved 2026-10-19.
  14. ↑ Shree K. Nayar (1997). "Catadioptric omnidirectional camera". Proceedings of the IEEE Computer Society Conference on Computer Vision and Pattern Recognition (CVPR 1997). IEEE. pp. 482-488. doi:10.1109/CVPR.1997.609369. https://doi.org/10.1109/CVPR.1997.609369. Retrieved 2026-10-19.
  15. ↑ Christopher Geyer, Kostas Daniilidis (2000). "A Unifying Theory for Central Panoramic Systems and Practical Applications". Computer Vision - ECCV 2000, Lecture Notes in Computer Science. Springer. pp. 445-461. doi:10.1007/3-540-45053-X_29. https://mlanthology.org/eccv/2000/geyer2000eccv-unifying. Retrieved 2026-10-19.
  16. ↑ Luis E. Gurrieri, Eric Dubois (2013-07-08). "Acquisition of omnidirectional stereoscopic images and videos of dynamic scenes: a review". Journal of Electronic Imaging, vol. 22, no. 3, article 030902. doi:10.1117/1.JEI.22.3.030902. https://ruor.uottawa.ca/items/8b06d98c-a150-4e12-9872-8e1cc3739a27. Retrieved 2026-10-19.
  17. ↑ 17.0 17.1 Yannanqi Li, Tao Zhan, Zhiyong Yang, Chi Xu, Patrick L. LiKamWa, Kun Li, Shin-Tson Wu (2021-02-09). "Broadband cholesteric liquid crystal lens for chromatic aberration correction in catadioptric virtual reality optics". Optics Express, vol. 29, no. 4. pp. 6011-6020. doi:10.1364/OE.419595. https://doi.org/10.1364/OE.419595. Retrieved 2026-10-19.
  18. ↑ Joseph A. LaRussa, Arthur T. Gill (1978-12-22). "The Holographic Pancake Window". Proceedings of SPIE, vol. 0162, Visual Simulation and Image Realism I. pp. 120-129. doi:10.1117/12.956898. https://doi.org/10.1117/12.956898. Retrieved 2026-10-19.
  19. ↑ Ziyu Wang, Liao Wang, Fuqiang Zhao, Minye Wu, Lan Xu, Jingyi Yu (2021-04-06). "MirrorNeRF: One-shot Neural Portrait Radiance Field from Multi-mirror Catadioptric Imaging". arXiv:2104.02607 [cs.CV]. https://arxiv.org/abs/2104.02607. Retrieved 2026-10-19.