Apodization of the incident light beam by an optimized quasi-Gaussian profile shifted along an aperture of the acousto-optical cell with appreciable acoustic losses

2012 ◽  
Author(s):  
Alexandre S. Shcherbakov ◽  
Alexander Laskin ◽  
Ana Virginia Hanessian de la Garza
1995 ◽  
Vol 25 (6) ◽  
pp. 582-586 ◽  
Author(s):  
O Parriaux ◽  
V A Sychugov ◽  
A V Tishchenko

2000 ◽  
Vol 78 (5-6) ◽  
pp. 537-542
Author(s):  
G Z Zhang

A method to increase the diffraction efficiency for optical gratings is proposed. Using a simple glass plate sitting parallel to the top of a grating surface, one can form an air gap between the surfaces of the grating and the glass plate to reflect a grazing-incident light beam and make diffraction through multiple reflection of the beam between the grating and glass plate surfaces. As a result, this device can efficiently enhance the grating efficiency by diffracting the input beam energy into various diffraction orders. PACS Nos.: 07.60-j, 42.25Fx, 42.40Lx, 42.79Dj, 42.40Fg


2016 ◽  
Vol 24 (3) ◽  
Author(s):  
P. Pura-Pawlikowska ◽  
M. Dudek ◽  
R. Wonko ◽  
P. Marć ◽  
M. Kujawińska ◽  
...  

AbstractWe present a micrometer-size polymer converter (microbridge) for connecting polymer optical fibres with silica fibres. The procedure of preparing such microstructure is based on a process of photopolymerization. A polymer converter grows as an extension of the fibres’ cores due to a self-guiding effect of the light beam in a photopolymerizable medium. Since the polymer microbridge has refractive index greater inside than outside, such a structure works as a waveguide leading the light beam between connected optical fibres. By selection of time of light exposition to the mixture and optical power of the incident light beam, it is possible to obtain a polymer converter with very good optical and mechanical characteristics. Possibility of using polymer microbridges grown directly from the fibres’ core as coupling elements between silica and polymer fibres is a good alternative for obtaining permanent coupling of such fibres.


Photoniques ◽  
2020 ◽  
pp. 59-64
Author(s):  
Aurélie Jullien

Spatial Light Modulators (SLMs) are quasiplanar devices, allowing for the modulation of the amplitude, phase and polarization, or a combination of these parameters of an incident light beam according to the two spatial dimensions of the modulator. SLMs are employed in many different fields and are the subject of continuous technological development.


PeerJ ◽  
2018 ◽  
Vol 6 ◽  
pp. e4482 ◽  
Author(s):  
Alexander V. Tschulakow ◽  
Theo Oltrup ◽  
Thomas Bende ◽  
Sebastian Schmelzle ◽  
Ulrich Schraermeyer

Objective In the foveola of the eye, photoreceptors and Müller cells with a unique morphology have been described, but little is known about their 3D structure and orientation. Considering that there is an angle-dependent change in the foveolar photoreceptor response for the same light beam, known as the Stiles Crawford Effect of the first kind (SCE I), which is still not fully understood, a detailed analysis of the anatomy of the foveolar cells might help to clarify this phenomenon. Methods Serial semithin and ultrathin sections, and focused ion beam (FIB) tomography were prepared from 32 foveolae from monkeys (Macaca fascicularis) and humans. Foveolae were also analyzed under the electron microscope. Serial sections and FIB analysis were then used to construct 3D models of central Müller and photoreceptor cells. In addition, we measured the transmission of collimated light under the light microscope at different angles after it had passed through human foveae from flat mounted isolated retinae. Results In monkeys, outer segments of central foveolar cones are twice as long as those from parafoveal cones and do not run completely parallel to the incident light. Unique Müller cells are present in the central foveolae (area of 200 µm in diameter) of humans and monkeys. Light entering the fovea center, which is composed only of cones and Müller cells, at an angle of 0° causes a very bright spot after passing through this area. However, when the angle of the light beam is changed to 10°, less light is measured after transpasssing through the retina, the foveolar center becomes darker and the SCE-like phenomenon is directly visible. Measurements of the intensities of light transmission through the central foveola for the incident angles 0 and 10° resemble the relative luminance efficiency for narrow light bundles as a function of the location where the beam enters the pupil as reported by Stiles and Crawford. The effect persisted after carefully brushing away the outer segments. Conclusion We show that unique cones and Müller cells with light fibre-like properties are present in the center of the fovea. These unique Müller cells cause an angle dependent, SCE-like drop in the intensity of light guided through the foveola. Outer segments from the foveolar cones of monkeys are not straight.


Author(s):  
Chia-Wen Lee ◽  
Chung-Feng Lai ◽  
Weileun Fang

Presently, various micromachined actuators have been employed to tune the tracking and focusing of the light beam of optical pick-up head [1–2]. This work demonstrates a novel micro-focusing stage for optical pick-up head application. As in Fig. 1a, the presented micro-focusing stage for optical pick-up head is consisted of four parts: out-of-plane actuator, connecting joint, through hole, and focusing lens plate. The stress-induced beams acted as the self-assembly mechanism to lift up focusing lens plate. In addition, the stress-induced beams also acted as the out-of-plane electrostatic actuator after deposited with an electrode layer. Unlike the design in [3], a through hole underneath the lens plate is allowed in this case for the incident light beam. After properly driving the stress-induced beams, the position of the focusing plate was controlled, as shown in Fig. 1b. The stage had piston motion to adjust the focal point of the lens. Moreover, the stage had tilt motion, so as to ensure that the lens paralleled the disk surface. Thus, the incident laser beam was always orthogonal with the disk surface.


2010 ◽  
Vol 12 (4) ◽  
pp. 045203 ◽  
Author(s):  
Alexandre S Shcherbakov ◽  
D Sanchez Lucero ◽  
A Luna Castellanos ◽  
Olga I Belokurova

1984 ◽  
Vol 62 (7) ◽  
pp. 661-668 ◽  
Author(s):  
Adelsindo Liberato de Brito ◽  
Arthur Jabs

We point out that the spectral width of a quasimonochromatic light beam broadens when the beam is focused. A quantitative formula for this broadening is derived from classical wave theory. The effect is shown to explain some experiments on laser beams done by Panarella which he explained using the ad hoc hypothesis that the frequency of the photons changes along with the intensity of the light beam. The line broadening by focusing might also contribute to gas ionization by incident light when the ionization potential is well above the mean photon energy. Remarks are made on some direct applications of the Heisenberg relations in comparison with our treatment.


Sensors ◽  
2020 ◽  
Vol 20 (4) ◽  
pp. 1218
Author(s):  
Yongbeom Lee ◽  
Keekeun Lee

An acousto-optic (AO) holographic display unit based on a suspended waveguide membrane was developed. The AO unit consists of a wide bandwidth chirp interdigital transducer (IDT) on a 20 µm thick suspended crystalline 128° YX LiNbO3 membrane, a light blocker with a 20 µm hole near the entrance, and an active lens near the exit. The 20 µm thickness of the floating membrane significantly enhanced surface acoustic wave (SAW) confinement. The light blocker was installed in front of the AO unit to enhance the coupling efficiency of the incident light to the waveguide membrane and to remove perturbations to the photodetector during measurement at the exit region. The active lens was vertically attached to the waveguide sidewall to collect the diffracted beam without loss and to modulate the focal length in free space through the applied voltage. As SAWs were radiated from the IDT, a Bragg grating with periodic refractive indexes was formed along the waveguide membrane. The grating diffracted incident light. The deflection angle and phase, and the intensity of the light beam were controlled by the SAW frequency and input power, respectively. The maximum diffraction efficiency achieved was approximately 90% for a 400 MHz SAW. COMSOL simulation and coupling of mode modeling were performed to optimize design parameters and predict device performance.


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