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Caption Article Title Author Name All

ALL IMAGES 1,225,629 You selected Adv. Opt. Photon. Adv. Opt. Photon.[Remove]
(4,705) Applied Optics Applied Optics[Remove] (399,484) Biomed. Opt.
Express Biomed. Opt. Express[Remove] (32,440) J. Opt. Commun. Netw. J. Opt.
Commun. Netw.[Remove] (17,159) JOSA JOSA[Remove] (54,227) JOSA A JOSA A[Remove]
(82,045) JOSA B JOSA B[Remove] (95,652) Optica Optica[Remove] (8,769) Opt.
Mater. Express Opt. Mater. Express[Remove] (23,437) Optics Express Optics
Express[Remove] (342,351) Optics Letters Optics Letters[Remove] (148,360) OSA
Continuum OSA Continuum[Remove] (7,393) Photonics Research Photonics
Research[Remove] (9,607)



 VOLUME     ISSUE     PAGE



DATE RANGE 1,225,629
1917

2021

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Browse and search more than 1 million images from Optica Publishing Group's core
journals. New images as soon are new articles are published.

Source: Nils J. Krichel, Aongus McCarthy, Gerald S. Buller, "Resolving range
ambiguity in a photon counting depth imager operating at kilometer distances,"
Opt. Express 18(9) 9192-9206 (2010);
https://www.osapublishing.org/oe/abstract.cfm?URI=oe-18-9-9192

Caption: 20 × 24 pixel scan of a life-size mannequin at 324 m distance. fSample
= 2 GHz, 7 × 106 pulses s−1, 16 ps histogram binning size, pattern length b =
16384 bits, 2 s per-pixel dwell time. Measurement acquired using a
shallow-junction SPAD. (a) Close-up photograph of the scene. (b) Segmented
surface plot of the scan, including several pixels locking onto background
objects.
Source: Cheng-Chien Liu, Po-Li Chen, "Automatic extraction of ground control
regions and orthorectification of remote sensing imagery," Opt. Express 17(10)
7970-7984 (2009);
https://www.osapublishing.org/oe/abstract.cfm?URI=oe-17-10-7970

Caption: The orthorectified aerial image and 5m DEM of Chiu-Shui River.
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);
https://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: X. F. Meng, X. Peng, L. Z. Cai, A. M. Li, J. P. Guo, Y. R. Wang,
"Wavefront reconstruction and three-dimensional shape measurement by two-step
dc-term-suppressed phase-shifted intensities," Opt. Lett. 34(8) 1210-1212
(2009);
https://www.osapublishing.org/ol/abstract.cfm?URI=ol-34-8-1210

Caption: Experimental results using the proposed method: some typical 3-D
geometries of the human face mask in wireframe mode.
Source: Maciej Antkowiak, Maria Leilani Torres-Mapa, Kishan Dholakia, Frank J.
Gunn-Moore, "Quantitative phase study of the dynamic cellular response in
femtosecond laser photoporation," Biomed. Opt. Express 1(2) 414-424 (2010);
https://www.osapublishing.org/boe/abstract.cfm?URI=boe-1-2-414

Caption: Comparison of quantitative phase maps with fluorescent assays during an
optoinjection experiment: a) phase map and b) propidium iodide fluorescence
(optoinjection assay) 5 min after irradiation ; c) phase map and d) Calcein AM
fluorescence (viability assay) after 90 min incubation. Two cells were
successfully optoinjected - one proved viable (solid arrow) while the other
(dashed arrow) was necrotic after 90 min. Note the significant decrease in the
optical thickness of the non-viable cell. Scale bars 20 μm.
Source: Jason Geng, "Structured-light 3D surface imaging: a tutorial," Adv. Opt.
Photon. 3(2) 128-160 (2011);
https://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: Adam K. Glaser, Ye Chen, Jonathan T. C. Liu, "Fractal propagation method
enables realistic optical microscopy simulations in biological tissues," Optica
3(8) 861-869 (2016);
https://www.osapublishing.org/optica/abstract.cfm?URI=optica-3-8-861

Caption: (a)–(d) x–z cross sections of the beam intensity are shown as a
function of focal depth, zf, for a focused Gaussian beam propagating through in
silico fractal medium 2. For each panel, the result for a single simulation is
displayed on top, with the corresponding averaged result over N=100 randomly
generated fractal media displayed on the bottom. For visualization, all images
are self-normalized to a maximum value of 1.
Source: Cleberson R. Alves, Alcenisio J. Jesus-Silva, Eduardo J. S. Fonseca,
"Robustness of a coherence vortex," Appl. Opt. 55(27) 7544-7549 (2016);
https://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: Nicolas Bonod, Jérôme Neauport, "Diffraction gratings: from principles
to applications in high-intensity lasers," Adv. Opt. Photon. 8(1) 156-199
(2016);
https://www.osapublishing.org/aop/abstract.cfm?URI=aop-8-1-156

Caption: Photograph of two large-area 1780 lines/mm diffraction gratings ( 420
   mm × 450    mm ) used at high incidence in a pulse compressor for the
high-energy PETAL laser [79]. The diffraction gratings are made of dielectrics;
see Section 6.1b.
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);
https://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: 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);
https://www.osapublishing.org//abstract.cfm?URI=---328

Caption:
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);
https://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.

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