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Development of a process for characterization of Nd:YAG crystals
Development of a process for characterization of Nd:YAG crystals

CRANFIELD UNIVERSITY Edouard Berrocal MULTIPLE
CRANFIELD UNIVERSITY Edouard Berrocal MULTIPLE

OPTICAL AND PASSIVATION PROPERTIES OF DOUBLE LAYER A
OPTICAL AND PASSIVATION PROPERTIES OF DOUBLE LAYER A

... ABSTRACT: The goal of this work is to study main trends regarding the transmittance and passivation properties of SiNy/a-Si:H ARC structures by variation and adjusting of the a-Si:H layer thickness. Experimental results on the transmittance for SiNx/a-Si:H/glass, a-Si:H/glass, SiNx/glass and on the ...
Fundamentals of Light Microscopy and Electronic Imaging
Fundamentals of Light Microscopy and Electronic Imaging

... economy and esthetic beauty of optical laws and principles. If carried out, the demonstrations and exercises also offer opportunities to become acquainted with new biological specimens that the reader may not have confronted or seen before by a new mode of light microscopy. Lists of materials, proce ...
Biomedical Optical Imaging
Biomedical Optical Imaging

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

Introduction to DWDM Technology
Introduction to DWDM Technology

optical guided waves and devices - Workspace
optical guided waves and devices - Workspace

... Another common component format, which offers a solution to some of these problems, is provided by integrated optics. As the name implies, this allows a number of guided wave devices to be combined on a common substrate. In contrast to optical fibre devices, integrated optic components are made usin ...
POLITECNICO DI MILANO Polo Regionale di Lecco Faculty of
POLITECNICO DI MILANO Polo Regionale di Lecco Faculty of

Strehl ratio for primary aberrations: some analytical results for
Strehl ratio for primary aberrations: some analytical results for

... first kind.8 However, this series converges rapidly, and only a few terms need be considered for adequate precision. The Strehl ratio for classical astigmatism is derived in Appendix A as an example of the results given in Table 1. The results for curvature of field or defocus and distortion or tilt ...
Topics in Adaptive Optics
Topics in Adaptive Optics

Multiterawatt few-cycle pulse OPCPA
Multiterawatt few-cycle pulse OPCPA

Laser and Gaussian Beam Propagation and Transformation
Laser and Gaussian Beam Propagation and Transformation

... same for any meridional plane containing the axis of propagation. Indeed, we did an easy calculation of the encircled energy for a circular beam by using these symmetry considerations (see Fig. 3). However, this is not the general case for a Gaussian beam.[39–41] For example, when a beam is transfor ...
Optical Pumping
Optical Pumping

... X. Other Optically Pumped Atoms. . . . . . . . . . . . . . . . . . . 237 pumping can also be detected by observing the AuoresA. Metastable States of the Heavy Noble Gases. . . . 237 cent light or byguoresceece moriitoring Ther. e are many B. Iead. . . . . . . . . . . . , . . . . . . . . . . . . . . ...
Laser Sources for Confocal Microscopy
Laser Sources for Confocal Microscopy

... In general, confocal microscopes work best at <1 mW of continuous wave (CW) beam power at the specimen and useful images of living cells have been made with <100 nW (see Chapter 19, this volume). When pulsed lasers are used for two-photon excitation it is important for the pulse frequency to be high ...
Integration of Magneto Optical Traps in Atom Chips
Integration of Magneto Optical Traps in Atom Chips

Laser Sources for Confocal Microscopy
Laser Sources for Confocal Microscopy

Full text - Simon Fraser University
Full text - Simon Fraser University

... and wax substrates. Raman studies of the ultrathin layers of MoS2 were carried out to characterize the thickness. During Raman measurement, an anomaly occurs: the strongest Raman intensity appears at a finite thickness of the MoS2 , a phenomenon also seen in graphite. A previous work [Y. Y. Wang et a ...
Modal Analysis and Controls Laboratory
Modal Analysis and Controls Laboratory

... OFDR measurement system. The light from a swept-tunable laser is split between a reference and measurement path of an interferometer using a fiber optic coupler. The light in the measurement path is sent to the fiber under test along the input port of an optical circulator. The light reflected from ...
Inverse Problems In Multiple Light Scattering
Inverse Problems In Multiple Light Scattering

... A common way to describe the wave interaction with disordered media is through Boltzmann theory for incoherent transport, which implicitly includes an average over all possible realizations of disorder and neglects possible interference effects [1]. The outcome is characterized statistically through ...
Final report
Final report

... been exploited for fibre optics-based sensing although silk fibres directly obtained from spiders can guide light and have shown early promises to being sensitive to some solvents. The aim of Silky Way, which is to demonstrate the proof-of-concept of fibre optic biosensors based on a single strand of ...
NGAO NGS WFS design review - Caltech Optical Observatories
NGAO NGS WFS design review - Caltech Optical Observatories

... any star in a 60x40 arcsecond Field of Regard • Whole WFS motion – the WFS must work with and without the IF dichoric • Lenslet XY motion & post-lenslet relay and camera focus – the WFS needs to operate in 63x63, 5x5 and pupil imaging modes. ...
Thursday, May 10, 2007
Thursday, May 10, 2007

The Strontium Optical Lattice Clock
The Strontium Optical Lattice Clock

... microwave clocks have demonstrated impressive frequency measurement accuracy, with fractional uncertainties below the 10−15 level. On the other hand, frequency standards based on optical transitions have made substantial steps forward over the last decade, benefiting from their high operational freq ...
The Strontium Optical Lattice Clock
The Strontium Optical Lattice Clock

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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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