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Optics and Quantum Electronics—J. G. Fujimoto, H. A. Haus, E. P. Ippen, F. X. Kärtner
Optics and Quantum Electronics—J. G. Fujimoto, H. A. Haus, E. P. Ippen, F. X. Kärtner

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Development of a high precision interferometric set-up for the

Modes Effective Refractive Index Difference Measurement
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253.pdf
253.pdf

Untitled
Untitled

... methods developed and used by various communities pursuing different applications. Topics include AO systems/component technologies, wavefront correction optics, control algorithms, and signal processing electronics used in adaptive optic implementations as well as limitations and novel applications ...
High efficiency high power blue laser by resonant doubling in PPKTP.
High efficiency high power blue laser by resonant doubling in PPKTP.

Optical coherence tomography (OCT): a review
Optical coherence tomography (OCT): a review

Distributed Temperature Sensing Using Stimulated
Distributed Temperature Sensing Using Stimulated

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... and (IV-164) propagates undistorted in the presence of dispersion and nonlinearity of opposite sign in optical fibers and are called an optical soliton. The word soliton refers to special kinds of wave packets that can propagate over long distances. Solitons have been discovered in many branches of ...
Optical frequency modulated continuous wave (FMCW) range and
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... and exposure time determines if a system is eye safe. Lasers are commonly classified as either class 1, 2, 3A, 3B or 4. A class 1 laser is totally safe, but the diffuse reflection from a class 4 laser damages the eye and the direct beam burns skin and ignites flammable material. In recent years, the ...
D12 in docx
D12 in docx

Optical properties of small-bore hollow glass waveguides
Optical properties of small-bore hollow glass waveguides

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Bandgap-assisted surface-plasmon sensing Arnaud J. Benahmed* and Chih-Ming Ho

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Recent Advances in High-Birefringence Fiber Loop Mirror Sensors

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c =λ* f λ = wavelength

Analysis of optical interferometric displacement detection in nanoelectromechanical systems
Analysis of optical interferometric displacement detection in nanoelectromechanical systems

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Numerical Analysis of Orbital Angular Momentum Based Next

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Vierbundelmenging in siliciumgebaseerde nanofotonische circuits

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IOSR Journal of Applied Physics (IOSR-JAP)
IOSR Journal of Applied Physics (IOSR-JAP)

A minimally invasive in-fibre Bragg grating sensor
A minimally invasive in-fibre Bragg grating sensor

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High-power, fiber-laser-pumped optical parametric oscillators from

... Abstract High-power, continuous-wave (cw), mid-infrared (mid-IR) laser sources are of interest for variety of applications such as trace gas detection and remote sensing, which require broad spectral coverage to address the most prominent absorption features of a wide range of molecular species pa ...
PDF
PDF



... Abstract High-power, continuous-wave (cw), mid-infrared (mid-IR) laser sources are of interest for variety of applications such as trace gas detection and remote sensing, which require broad spectral coverage to address the most prominent absorption features of a wide range of molecular species pa ...
Waveguide Dispersion
Waveguide Dispersion

... Combining intermodal and intramodal dispersions Consider a graded index fiber with a core diameter of 30 mm and a refractive index of 1.474 at the center of the core and a cladding refractive index of 1.453. Suppose that we use a laser diode emitter with a spectral linewidth of 3 nm to transmit alo ...
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Optical amplifier



An optical amplifier is a device that amplifies an optical signal directly, without the need to first convert it to an electrical signal. An optical amplifier may be thought of as a laser without an optical cavity, or one in which feedback from the cavity is suppressed. Optical amplifiers are important in optical communication and laser physics.There are several different physical mechanisms that can be used to amplify a light signal, which correspond to the major types of optical amplifiers. In doped fibre amplifiers and bulk lasers, stimulated emission in the amplifier's gain medium causes amplification of incoming light. In semiconductor optical amplifiers (SOAs), electron-hole recombination occurs. In Raman amplifiers, Raman scattering of incoming light with phonons in the lattice of the gain medium produces photons coherent with the incoming photons. Parametric amplifiers use parametric amplification.
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