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Optics in Astronomy
Optics in Astronomy

... Concepts of coherence III • Coherence is a property of the e.m. field vector! • It is important to consider the state of polarisation of the light as orthogonal states of polarisation do not interfere (laws of Fresnel-Arago). • Optical designs of interferometers which change the state of polarisait ...
A Quantum Gas Microscope for Fermionic Atoms
A Quantum Gas Microscope for Fermionic Atoms

Optical field profile evaluation on silica high Optical field profile
Optical field profile evaluation on silica high Optical field profile

... from FFP are appared the difference in vicinity of boundary of core and clad of silicon waveguide (x = ±1.0µm). The optical field of NFP, resulting from the conversion of FFP correspond closely with the optical field of NFP simulated using FEM. The difference arises due to the approximation used in ...
Fiber Optics
Fiber Optics

... where a and no are the radius and refractive index at the center of the core, respectively. In the case of a parabolic index fiber (α = 2) the total power that can be launched is one half of that of a step-index fiber with the same ∆ (NA). Graded-index fibers are found in most applications for telec ...
Three-Dimensional Simulation of Vertical-Cavity Surface
Three-Dimensional Simulation of Vertical-Cavity Surface

... wavelength control and narrow optical linewidth. Although VCSELs might improve on some aspects, there is little pressure on this low-volume market to drive the development of cheaper optical sources. However, long wavelength single-mode VCSELs could be more promising than the recent Fabry-Perot lase ...
Optical Breakdown in Liquid Suspensions and Its Analytical
Optical Breakdown in Liquid Suspensions and Its Analytical

Simulation of Fiber Fuse Phenomenon in Single
Simulation of Fiber Fuse Phenomenon in Single

... Ge-doped silica core at 2,293 K was assumed to be 5.6 ×104 m−1 at 0.5 µm [5]. This large α value, however, could not be estimated using their Arrhenius equation [6]. As the focal length F of thermal lense effect is inversely as the α value [63], large α value of 5.6 ×104 m−1 is necessary to obtain s ...
Final Thesis_Compatible Mode
Final Thesis_Compatible Mode

Physical properties of silver oxide thin films by pulsed laser deposition
Physical properties of silver oxide thin films by pulsed laser deposition

... tetragonal [5–7]. Silver oxide thin films have been prepared by several techniques: RF and dc sputtering [8, 9], thermal evaporation [10], chemical synthesis [2] and by pulsed laser deposition (PLD) [11]. Our earlier studies [8] on silver oxide thin films prepared by the reactive dc magnetron sputte ...
UNIVERSIDAD DE MURCIA ABERRACIONES EN LENTES OFTÁLMICAS DE POTENCIA
UNIVERSIDAD DE MURCIA ABERRACIONES EN LENTES OFTÁLMICAS DE POTENCIA

Theoretical and empirical comparison of coupling coefficient and
Theoretical and empirical comparison of coupling coefficient and

1378120180.
1378120180.

... Conjugated foci. ...
WAVE INTERACTIONS WITH ARRAYS OF BOTTOM
WAVE INTERACTIONS WITH ARRAYS OF BOTTOM

Quantum theory of high-resolution length measurement with a Fabry
Quantum theory of high-resolution length measurement with a Fabry

INFLUENCE OF OPTICAL PROPERTIES AND FIBERSEPARATION ON LASER DOPPLER FLOWMETRY
INFLUENCE OF OPTICAL PROPERTIES AND FIBERSEPARATION ON LASER DOPPLER FLOWMETRY

... theoretically using either a Monte Carlo simulation model4, 5 or a lattice random-walk model6. The latter two reports did not only show that the sampling depth increases with fiber separation but also that the it is affected by the optical properties of the tissue. In addition, Weiss et al. shows th ...
Advance Program Sunday, October 12, 2014 Sunday Session
Advance Program Sunday, October 12, 2014 Sunday Session

guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America

... Example: If an object is placed at a distance of 33 mm in front of a biconvex lens with a focal length of 30 mm, the lens will produce a 10-times magnified image (M = 10:1) at a distance of 330 mm behind the lens. The human eye can modify the focal length by changing the curvature of its lens such t ...
Extended Nijboer-Zernike representation of the vector field in the
Extended Nijboer-Zernike representation of the vector field in the

Porous Waveguide in the Kretschmann Configuration for Small Molecule Detection
Porous Waveguide in the Kretschmann Configuration for Small Molecule Detection

Fiber Optic Lab Manual
Fiber Optic Lab Manual

... This manual is an action-filled guide for completing nine stimulating activities related to fiber optic communications. The manual is compatible with most classroom texts and is ideal for creating a lab to go with almost any vocational or secondary-education fiber optics course. For best results we ...
Fiber optic Fabry-Perot interferometer for
Fiber optic Fabry-Perot interferometer for

... A general optical fiber sensors classification differentiates intrinsic and extrinsic types. When light is modified outside fiber´s material then it is called extrinsic, on the other hand when light is modified inside the fiber it is the intrinsic type of sensor. Intrinsic sensors are commonly used ...
Get PDF - OSA Publishing
Get PDF - OSA Publishing

... EIT-based nonlinear schemes can be driven by traveling wave beams as well as by a standing wave (SW). The large nonlinearity was obtained in an atomic system driven by two counter propagating coupling fields which form a SW if the two counter propagating coupling fields have the same frequency [11, ...
Experimental and Theoretical Studies in Optical Coherence Theory
Experimental and Theoretical Studies in Optical Coherence Theory

Metal-optic and Plasmonic Semiconductor
Metal-optic and Plasmonic Semiconductor

The Sampling Pattern Cube
The Sampling Pattern Cube

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Retroreflector



A retroreflector (sometimes called a retroflector or cataphote) is a device or surface that reflects light back to its source with a minimum of scattering. In a retroreflector an electromagnetic wavefront is reflected back along a vector that is parallel to but opposite in direction from the wave's source. The angle of incidence at which the device or surface reflects light in this way is greater than zero, unlike a planar mirror, which does this only if the mirror is exactly perpendicular to the wave front, having a zero angle of incidence.
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