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. 3(2) 128-160 (2011);
http://www.osapublishing.org/aop/abstract.cfm?URI=aop-3-2-128

Caption: Example of color stripe indexing based on De Bruijn sequence ( k = 5 , n = 3 )  [35].

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: Andreas Rottler, Stephan Schwaiger, Aune Koitmäe, Detlef Heitmann, Stefan Mendach, "Transmission enhancement in three-dimensional rolled-up plasmonic metamaterials containing optically active quantum wells," J. Opt. Soc. Am. B 28(10) 2402-2407 (2011);
http://www.osapublishing.org/josab/abstract.cfm?URI=josab-28-10-2402

Caption: Sketch of a microroll that can be fabricated by rolling up strained layers. The tube wall represents a three- dimensional metamaterial consisting of a metal–semiconductor superlattice containing quantum wells and metal gratings.

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.

Source: Afshin Moradi, "Plasmon hybridization in coated metallic nanowires," J. Opt. Soc. Am. B 29(4) 625-629 (2012);
http://www.osapublishing.org/josab/abstract.cfm?URI=josab-29-4-625

Caption: Plasmon energy ω in electron volts of a composite gold NT and gold core system, for q=0 and m=2, using ωp=1.37×1016  Hz, plotted versus δ and d, when a1=7  nm.

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: C. R. Phillips, M. M. Fejer, "Stability of the singly resonant optical parametric oscillator," J. Opt. Soc. Am. B 27(12) 2687-2699 (2010);
http://www.osapublishing.org/josab/abstract.cfm?URI=josab-27-12-2687

Caption: Normalized net round-trip gain G s p as a function of pump-signal and idler-signal phase mismatches δ ν p s Ω L and δ ν i s Ω L , respectively, for N = ( π / 2 ) 2 . GVD is neglected, so the AM and PM eigenmodes are decoupled. (a) Gain for AM eigenmodes, (b) gain for PM eigenmodes.

Source: Andrew Forbes, Angela Dudley, Melanie McLaren, "Creation and detection of optical modes with spatial light modulators," Adv. Opt. Photon. 8(2) 200-227 (2016);
http://www.osapublishing.org/aop/abstract.cfm?URI=aop-8-2-200

Caption: Liquid-crystal SLMs allow unprecedented control in the generation and detection of structured light fields. (a) Long exposure image of laser light diffracted from the pixelated device. (b) CCD camera image showing the various diffraction orders. Efficiencies are typically in the 60%–85% range.

Source: Cleberson R. Alves, Alcenisio J. Jesus-Silva, Eduardo J. S. Fonseca, "Robustness of a coherence vortex," Appl. Opt. 55(27) 7544-7549 (2016);
http://www.osapublishing.org/ao/abstract.cfm?URI=ao-55-27-7544

Caption: Experimental results of the signal and reference speckled beams with triangular aperture and cross-correlations between them in the first, second, and third columns, respectively.

Source: Chan M. Lim, G. Hugh Song, "Design of superperiodic photonic-crystal light-emitting plates with highly directive luminance characteristics," J. Opt. Soc. Am. B () 328-336 (2000);
http://www.osapublishing.org//abstract.cfm?URI=---328

Caption:

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.