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: 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: Christian Kränkel, Rigo Peters, Klaus Petermann, Pascal Loiseau, Gerard Aka, Günter Huber, "Efficient continuous-wave thin disk laser operation of $\text{Yb}:{\text{Ca}}_4\text{YO}{\left({\text{BO}}_3\right)}_3$ in $\mathbf{E}\parallel \mathbf{Z}$ and $\mathbf{E}\parallel \mathbf{X}$ orientations with 26 W output power," J. Opt. Soc. Am. B 26(7) 1310-1314 (2009);
http://www.osapublishing.org/josab/abstract.cfm?URI=josab-26-7-1310

Caption: Schematic setup of the thin disk laser resonator and the pump module.

Source: Yinan Zhang, Marko Lončar, "Submicrometer diameter micropillar cavities with high quality factor and ultrasmall mode volume," Opt. Lett. 34(7) 902-904 (2009);
http://www.osapublishing.org/ol/abstract.cfm?URI=ol-34-7-902

Caption: (a) Schematic of a four-taper-segment micropillar cavity. (b) and (c) Electric field density profile of the first- and second-order modes, respectively. (d) Electric field density profile of the third-order mode of the ten-taper-segment micropillar cavity. (e) Mode diagram as a function of taper segment number.

Source: Suxia Xie, Hongjian Li, Xin Zhou, Haiqing Xu, Zhimin Liu, "Tunable optical transmission through gold slit arrays with Z-shaped channels," J. Opt. Soc. Am. A 28(3) 441-447 (2011);
http://www.osapublishing.org/josaa/abstract.cfm?URI=josaa-28-3-441

Caption: Transmission spectra through a lattice of periodic gold film perforated with Z-shaped slits with slit widths w 2 = 25 , 50, 100, 150   nm . h = 500   nm , l = 800   nm , s 2 = 450   nm , w 1 = w 3 = 150   nm .

Source: Pengcheng Li, Celong Liu, Xianpeng Li, Honghui He, Hui Ma, "GPU acceleration of Monte Carlo simulations for polarized photon scattering in anisotropic turbid media," Appl. Opt. 55(27) 7468-7476 (2016);
http://www.osapublishing.org/ao/abstract.cfm?URI=ao-55-27-7468

Caption: GPU simulation results with the same parameters as in Fig. 4 of [9]. Thickness of the medium is 1 cm, refractive index n=1.33, wavelength of light is 633 nm. Radius, refractive index, and scattering coefficient of the spherical scatterer in the simulations in (a) and (b) are rs=0.1  μm, ns=1.59, μs=10  cm−1, and in the sphere–cylinder mixed simulations in (c) and (d), μs=5  cm−1. For the cylindrical scatterer in the simulations in (c) and (d), rc=0.75  μm, nc=1.56, μc(90°)=65  cm−1. The direction of the cylinders is along the y axis, and the standard deviation for the Gauss distribution of the direction is 5°. The birefringence value in the simulations in (b) and (d) is 1×10−5, corresponding to an extension of 5 mm. The birefringence axis is along the 45° direction on the x–y plane. The cutoff numbers of scattering steps are all set to 200. The number of simulated photons is 1.2×108 for each group. The detector area is 1  cm×1  cm, partitioned into 100×100 pixels.

Source: François Blanchard, Koichiro Tanaka, "Improving time and space resolution in electro-optic sampling for near-field terahertz imaging," Opt. Lett. 41(20) 4645-4648 (2016);
http://www.osapublishing.org/ol/abstract.cfm?URI=ol-41-20-4645

Caption: THz near-field images in the frequency domain. (a) and (b) Amplitude frequency maps at 300 GHz normalized to reference maps using 10- and 1-μm-thick X -cut LN crystals, respectively (visible image of the sample on the right hand side). (c)–(e) Expanded view for the conditions without probe filtering, with probe filtering using the 10-μm-thick sensor, and with probe filtering using the 1-μm-thick sensor, respectively (i.e., zones identified by the doted lines in the visible images).

Source: Xin Gai, Duk-Yong Choi, Steve Madden, Barry Luther-Davies, "Interplay between Raman scattering and four-wave mixing in ${\mathrm{As}}_2{\mathrm{S}}_3$ chalcogenide glass waveguides," J. Opt. Soc. Am. B 28(11) 2777-2784 (2011);
http://www.osapublishing.org/josab/abstract.cfm?URI=josab-28-11-2777

Caption: Numerical simulations of amplification of white noise by FWM and SRS as a function of propagation length.

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: 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: 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: Antony C. S. Chan, Kevin K. Tsia, Edmund Y. Lam, "Subsampled scanning holographic imaging (SuSHI) for fast, non-adaptive recording of three-dimensional objects," Optica 3(8) 911-917 (2016);
http://www.osapublishing.org/optica/abstract.cfm?URI=optica-3-8-911

Caption: Compressed spiral-scanning measurement and reconstruction of physical 3D object with spiral scanning. (Top row) Subsampled complex-valued hologram data along the spiral path. The magnitude and phase values are represented by the saturation and hue, respectively, as shown in the color wheel of the legend. Undefined hologram pixels are displayed as the gray color. The corresponding numbers of spiral revolutions p, compression ratio M/N, and the reconstruction performance score (SSIM) are shown in Table 1. (Bottom row) The reconstructed image shows the proximal layer in red (z1=870  mm) and the distal layer in blue (z2=1070  mm). Empty space is depicted as white. (Inset) The zoomed-in view of the restored 3D object. Note the high quality of letter “S” down at the 25% compression ratio.