OpticsInfoBase

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);
http://www.opticsinfobase.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: Jolly Xavier, Joby Joseph, "Tunable complex photonic chiral lattices by reconfigurable optical phase engineering," Opt. Lett. 36(3) 403-405 (2011);
http://www.opticsinfobase.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: 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.opticsinfobase.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: Alison M. Yao, Miles J. Padgett, "Orbital angular momentum: origins, behavior and applications," Adv. Opt. Photon. 3(2) 161-204 (2011);
http://www.opticsinfobase.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: Takashi Notake, Kouji Nawata, Hiroshi Kawamata, Takeshi Matsukawa, Hiroaki Minamide, "Solution growth of high-quality organic N-benzyl-2-methyl-4-nitroaniline crystal for ultra-wideband tunable DFG-THz source," Opt. Mater. Express 2(2) 119-125 (2012);
http://www.opticsinfobase.org/ome/abstract.cfm?URI=ome-2-2-119

Caption: Calculation result of prospective THz-wave intensity via BNA-DFG under the consideration of perfect phase matching and absorption effect.

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

Caption: 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.

Source: Jason Geng, "Structured-light 3D surface imaging: a tutorial," Adv. Opt. Photon. 3(2) 128-160 (2011);
http://www.opticsinfobase.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: 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.opticsinfobase.org//abstract.cfm?URI=---328

Caption:

Source: Jia Qin, Roberto Reif, Zhongwei Zhi, Suzan Dziennis, Ruikang Wang, "Hemodynamic and morphological vasculature response to a burn monitored using a combined dual-wavelength laser speckle and optical microangiography imaging system," Biomed. Opt. Express 3(3) 455-466 (2012);
http://www.opticsinfobase.org/boe/abstract.cfm?URI=boe-3-3-455

Caption: Co-registered image of the change in blood flow image (Fig. 3A) with the projection view image of the blood vessel network obtained by the OMAG method after the injury (Fig. 4B). The color map is the same as in Fig. 3A. The grayscale of the OMAG image was inverted such that the blood vessels appear dark for better contrast.

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

Caption: Normalized intensity (top) and phase (bottom) profiles of some superpositions of Laguerre–Gaussian modes: L G 01 + L G 05 , L G 0 − 5 + L G 05 , and L G 10 + L G 05 (left to right).

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.opticsinfobase.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.