Optics ImageBank

ALL IMAGES618,827
Adv. Opt. Photon.(985)
Applied Optics(264,341)
Biomed. Opt. Express(8,480)
J. Opt. Commun. Netw.(4,770)
JOSA A(65,729)
JOSA B(26,325)
Opt. Mater. Express(4,986)
Optics Express(168,918)
Optics Letters(74,293)
 VOLUME     ISSUE     PAGE
DATE RANGE 619,401
Click to choose OSA TECHNICAL DIVISIONS  
Click to choose OCIS CODES

Optics InfoBase > Optics ImageBank > HomeHome  |  About

1 Example of 2D array of color-coded dots.
2 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.
3 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 .
4 Calculation result of prospective THz-wave intensity via BNA-DFG under the consideration of perfect phase matching and absorption effect.
5 (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.
6 Transfer of angular momentum in optical tweezers. A trapped object can be rotated either by the transfer of SAM from a circularly polarized beam (left) or by the transfer of OAM from a high-order Laguerre–Gaussian beam.
7 Comparison of x-ray images of (a) cartilage on a chicken’s bone and (e) a tomato. The cartilage is shown clearly in (c) the differential phase image compared to (b) the absorption and (d) the scattering images. The inner structure of the tomato can be seen in (h) the scattering image, whereas (f) the absorption and (g) the differential phase images do not show any profiles.
8 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.
9 Experimental results using the proposed method: some typical 3-D geometries of the human face mask in wireframe mode.
10 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).
11 Normalized linear Stokes vector components demonstrate polarization synthesis.
12 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.