Source: Michael J. Murdoch, Ingrid E. J. Heynderickx, "Veiling glare and perceived black in high dynamic range displays," J. Opt. Soc. Am. A 29(4) 559-566 (2012);
http://www.osapublishing.org/josaa/abstract.cfm?URI=josaa-29-4-559

Caption: Source images used in the experiment. Upper, L-R: cosine, cosine2, curls. Lower, L-R: eye, nose, palm. Each image was presented at a size of two degrees of visual angle square.

Source: Jin Hou, Jiajia Zhao, Chunyong Yang, Zhiyou Zhong, Yihua Gao, Shaoping Chen, "Engineering ultra-flattened-dispersion photonic crystal fibers with uniform holes by rotations of inner rings," Photon. Res. 2(2) 59-63 (2014);
http://www.osapublishing.org/prj/abstract.cfm?URI=prj-2-2-59

Caption: Fundamental mode transverse electric field intensity (Et2) distributions at 1.45 μm (upper figures) and 1.75 μm (lower figures) wavelengths, for nearly zero-dispersion flattened PCFs with Λ=2.3  μm and d=0.61  μm for (a) α=0° and β=0°, (b) α=30° and β=0°, (c) α=0° and β=30°, (d) α=0° and β=0°, (e) α=30° and β=0°, and (f) α=0° and β=30°.

Source: Christoph J. Engelbrecht, Werner Göbel, Fritjof Helmchen, "Enhanced fluorescence signal in nonlinear microscopy through supplementary fiber-optic light collection," Opt. Express 17(8) 6421-6435 (2009);
http://www.osapublishing.org/oe/abstract.cfm?URI=oe-17-8-6421

Caption: Supplementary epifluorescence collection through a ring of optical fibers. (a) Top: CAD-drawing of a custom fiber-ring holder placed under an objective. Bottom: Closeup view showing the ring-like arrangement of the fiber tips. Only five of eight fibers are shown. Fluorophores are 2-photon excited in the focus of an infrared laser beam (red), causing isotropic fluorescence emission (green). (b) Left: Top view of the ring-like arrangement of eight 1-mm diameter fibers. Right: Dual-channel detection in a custom 2PLSM setup. Optical fibers were bundled and placed in front of a second PMT.

Source: Jason Geng, "Structured-light 3D surface imaging: a tutorial," Adv. Opt. Photon. () 128-160 (2000);
http://www.osapublishing.org//abstract.cfm?URI=---128

Caption:

Source: Patrick Robert Gill, Changhyuk Lee, Dhon-Gue Lee, Albert Wang, Alyosha Molnar, "A microscale camera using direct Fourier-domain scene capture," Opt. Lett. 36(15) 2949-2951 (2011);
http://www.osapublishing.org/ol/abstract.cfm?URI=ol-36-15-2949

Caption: Decomposition of natural images into Fourier components. (a) All images can be expressed as a sum of 2D Fourier basis functions [e.g., (b)] by taking the sum over all values in (c) the basis-scaled image.

Source: V. K. Valev, X. Zheng, C.G. Biris, A.V. Silhanek, V. Volskiy, B. De Clercq, O. A. Aktsipetrov, M. Ameloot, N. C. Panoiu, G. A. E. Vandenbosch, V. V. Moshchalkov, "The origin of second harmonic generation hotspots in chiral optical metamaterials [Invited]," Opt. Mater. Express 1(1) 36-45 (2011);
http://www.osapublishing.org/ome/abstract.cfm?URI=ome-1-1-36

Caption: Second harmonic generation methods for studying chirality were developed in organic molecules before being applied to metamaterials. In (a), illustration of SHG from supramolecularly ordered chiral helicenes molecules. In (b), illustration of SHG from G-shaped nanostructures, arranged in a chiral unit cell. The incoming light is at 800 nm (near red color) and the detected signal is at 400 nm (near blue color).

Source: Jason Geng, "Structured-light 3D surface imaging: a tutorial," Adv. Opt. Photon. 3(2) 128-160 (2011);
http://www.osapublishing.org/aop/abstract.cfm?URI=aop-3-2-128

Caption: Example of 2D array of color-coded dots.

Source: M. W. Holtfrerich, M. Dowran, R. Davidson, B. J. Lawrie, R. C. Pooser, A. M. Marino, "Toward quantum plasmonic networks," Optica 3(9) 985-988 (2016);
http://www.osapublishing.org/optica/abstract.cfm?URI=optica-3-9-985

Caption: Effect of EOT on spatial information. The central figure shows the input probe beam generated with the DLP before the FWM. The top row shows the entangled images generated by the FWM process before the plasmonic structures, while the lower row shows the entangled images after transduction through the plasmonic structures.

Source: Alison M. Yao, Miles J. Padgett, "Orbital angular momentum: origins, behavior and applications," Adv. Opt. Photon. 3(2) 161-204 (2011);
http://www.osapublishing.org/aop/abstract.cfm?URI=aop-3-2-161

Caption: Ghost imaging: coincidence measurements of two beams of entangled photons—one of which interacts with an object and one of which doesn’t—can be used to reconstruct a “ghost” image of the object.

Source: T. J. Eichelkraut, G. A. Siviloglou, I. M. Besieris, D. N. Christodoulides, "Oblique Airy wave packets in bidispersive optical media," Opt. Lett. 35(21) 3655-3657 (2010);
http://www.osapublishing.org/ol/abstract.cfm?URI=ol-35-21-3655

Caption: Isointensity plot of an oblique spatiotemporal Bessel–Airy wave packet.

Source: Yaroslav V. Kartashov, Chao Hang, Guoxiang Huang, Lluis Torner, "Three-dimensional topological solitons in $\mathcal{PT}$ -symmetric optical lattices," Optica 3(10) 1048-1055 (2016);
http://www.osapublishing.org/optica/abstract.cfm?URI=optica-3-10-1048

Caption: Profile of a stable l = + 1 vortex soliton with b = 4.4 , p i = 0.55 . Isosurface depicting the field modulus distribution (left) at | q | = 0.07 .

Source: Jolly Xavier, Joby Joseph, "Tunable complex photonic chiral lattices by reconfigurable optical phase engineering," Opt. Lett. 36(3) 403-405 (2011);
http://www.osapublishing.org/ol/abstract.cfm?URI=ol-36-3-403

Caption: Computer simulation of the light- intensity distribution of the interference pattern for hexagonal right-handed (RH) as well as left-handed (LH) photonic chiral structures using 6 + 1 beam geometry. (a) 3D interference intensity distribution for RH structures. (c) Intensity profile in x − z plane. (b) and (d) correspond to (a) and (c) for LH photonic chiral structures.