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Diode pumped distributed Bragg reflector lasers
Diode pumped distributed Bragg reflector lasers

Get PDF - OSA Publishing
Get PDF - OSA Publishing

Full Text  - Journal of The Royal Society Interface
Full Text - Journal of The Royal Society Interface

Raman Spectra of Optically Trapped Microcomplexes
Raman Spectra of Optically Trapped Microcomplexes

Helium-Neon Laser 1 Introduction
Helium-Neon Laser 1 Introduction

... of where the CCD array is located when positioning the camera with respect to the beam. Turn on the appropriate software and look at your beam. CCD’s have a certain saturation level beyond which there is only a fixed amount of signal registered. By using the right filters you will be able to achieve ...
Minimized speckle noise in lens-less holographic projection by pixel
Minimized speckle noise in lens-less holographic projection by pixel

... persistent difficulties with laser eye-safety and strong image flickering. On the other hand the holographic projection provides stable images formed by strongly divergent wavefronts, which ensures a completely safe operation. From the point of view of energetic efficiency, the utilization of 8-bit ...
Single Longitudinal Mode Blue-Violet Laser Diode for Data Storage
Single Longitudinal Mode Blue-Violet Laser Diode for Data Storage

Generalized Multiprotocol Label Switching: An Overview of Routing
Generalized Multiprotocol Label Switching: An Overview of Routing

Color center production by femtosecond-pulse laser
Color center production by femtosecond-pulse laser

b. optical wave breaking in the pcf
b. optical wave breaking in the pcf

... same measured SC (correspond to Fig.3(c), input peak power=118W) where the wavelength resolution is 0.01nm. As we magnify the horizontal axis of Fig.4(a), the microstructure of the spectrum become clearly, as shown in Fig.4(b). We note that the optical comb has the uniform precise channel spacing of ...
Determination of the transfer function for optical surface topography
Determination of the transfer function for optical surface topography

... so-called weak object transfer function (WOTF) is sometimes possible in a partially coherent system if scattering from the object can be considered weak [34]; however, this will not be discussed further here for the sake of brevity. Studies of OTFs were perhaps first initiated by Dändlinker and Wei ...
MONABIPHOT_All_Courses_2016
MONABIPHOT_All_Courses_2016

... Prerequisites : this course is intended towards student in need of an update in basic math. It does not require any special prerequisite . Prior to the course, screening tests will be organized to check on the level of students and orient them to this course when needed. Objectives : This course is ...
de Sénarmont Bias Retardation in DIC Microscopy Introduction
de Sénarmont Bias Retardation in DIC Microscopy Introduction

... impossible) to adapt a Wollaston prism for use with standard microscope objectives, which often have a rear focal plane (that must physically coincide with the Wollaston prism interference plane) buried deep inside a lens. Similar to a conventional Wollaston prism, the basic Nomarski prism design (F ...
Slide 1
Slide 1

L/f 1
L/f 1

Amplitude and Phase of Tightly Focused Laser Beams in Turbid Media
Amplitude and Phase of Tightly Focused Laser Beams in Turbid Media

Photofragmentation-laser induced fluorescence: a
Photofragmentation-laser induced fluorescence: a

... equal to or less than that of the PMT dark count via a combination of long wavelength chemical filters and solar blind PM tubes. The second subcategory of laser induced noise (i.e., sources that generate noise wavelengths
Tech Notes Wavelength 2012 | www.ll.mit.edu
Tech Notes Wavelength 2012 | www.ll.mit.edu

Handbook of Optical Filters for Fluorescence Microscopy
Handbook of Optical Filters for Fluorescence Microscopy

Two-dimensional control of light with light on metasurfaces
Two-dimensional control of light with light on metasurfaces

... of the standing wave results in fourfold enhancement or selection (recognition) of the logo’s central sun, which both images have in common (panel (c)). On the other hand, a π phase shift of one illuminating beam shifts the standing wave, placing the metasurface near an electric antinode, where the ...
External visual interface for a Nikon 6D autocollimator
External visual interface for a Nikon 6D autocollimator

... the Electronic Level was disregarded because this research is focused on the new instrument’s resolution. This indicates that errors in measurements using the camera plus the autocollimator ensemble are not random in nature. The discrepancies are define on: Dk = αk − (a ∗ Xk + b) ...
Distributed-gain measurements of erbium
Distributed-gain measurements of erbium

... capacity and functionality of optical networks. One of the key parameter in an EDFA fabrication is the ideal length of the doped fiber, which is normally calculated theoretically [1]-[2]. However, the practical determination of the optimum length for maximum gain is done with a cutback method, which ...
Exercice N°1 : Laser à 4 niveaux
Exercice N°1 : Laser à 4 niveaux

Variational Phase Imaging Using the Transport-of
Variational Phase Imaging Using the Transport-of

... Index Terms— Phase retrieval, transport-of-intensity equation, sparse reconstruction, total variation regularization, weightednorm regularization, phase imaging, phase microscope. ...
The wide blue yonder
The wide blue yonder

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Super-resolution microscopy

Super-resolution microscopy is a form of light microscopy. Due to the diffraction of light, the resolution of conventional light microscopy is limited as stated by Ernst Abbe in 1873. A good approximation of the resolution attainable is the full width at half maximum (FWHM) of the point spread function, and a precise widefield microscope with high numerical aperture and visible light usually reaches a resolution of ~250 nm.Super-resolution techniques allow the capture of images with a higher resolution than the diffraction limit. They fall into two broad categories, ""true"" super-resolution techniques, which capture information contained in evanescent waves, and ""functional"" super-resolution techniques, which use clever experimental techniques and known limitations on the matter being imaged to reconstruct a super-resolution image.True subwavelength imaging techniques include those that utilize the Pendry Superlens and near field scanning optical microscopy, the 4Pi Microscope and structured illumination microscopy technologies like SIM and SMI. However, the majority of techniques of importance in biological imaging fall into the functional category.There are two major groups of methods for functional super-resolution microscopy: Deterministic super-resolution: The most commonly used emitters in biological microscopy, fluorophores, show a nonlinear response to excitation, and this nonlinear response can be exploited to enhance resolution. These methods include STED, GSD, RESOLFT and SSIM. Stochastic super-resolution: The chemical complexity of many molecular light sources gives them a complex temporal behaviour, which can be used to make several close-by fluorophores emit light at separate times and thereby become resolvable in time. These methods include SOFI and all single-molecule localization methods (SMLM) such as SPDM, SPDMphymod, PALM, FPALM, STORM and dSTORM.On October 8th, 2014, the Nobel Prize in Chemistry was awarded to Eric Betzig, W.E. Moerner and Stefan Hell for ""the development of super-resolved fluorescence microscopy,"" which brings ""optical microscopy into the nanodimension"".
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