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The spectroscopic line shape of the CARS intensity therefore resembles a Fano profile which is shifted with respect to the Raman signal. To compare the spectra from multi-component compounds, the (resonant) CARS spectral amplitude should be compared to the Raman spectral intensity. Coherent anti-Stokes Raman spectrum of microscopy oil.
A common solution for this is fabricating the microfluidic device such that a confocal pinhole can be used for the Raman laser. [264] Typical confocal Raman microscopy allows for spectroscopic information from small focal volumes less than 1 micron cubed, and thus smaller than the microfluidic channel dimensions. [269]
Raman microscopy, and in particular confocal microscopy, can reach down to sub-micrometer lateral spatial resolution. [7] Because a Raman microscope is a diffraction-limited system, its spatial resolution depends on the wavelength of light and the numerical aperture of the focusing element. In confocal Raman microscopy, the diameter of the ...
PEEM – Photoemission electron microscopy (or photoelectron emission microscopy) PES – Photoelectron spectroscopy; PINEM – photon-induced near-field electron microscopy; PIGE – Particle (or proton) induced gamma-ray spectroscopy, see nuclear reaction analysis; PIXE – Particle (or proton) induced X-ray spectroscopy; PL – Photoluminescence
Fluorescence and confocal microscopes operating principle. Confocal microscopy, most frequently confocal laser scanning microscopy (CLSM) or laser scanning confocal microscopy (LSCM), is an optical imaging technique for increasing optical resolution and contrast of a micrograph by means of using a spatial pinhole to block out-of-focus light in image formation. [1]
SRS and CARS were theoretically predicted and experimentally realized in the 1960s. [1] [2] [3] In 1982 the first CARS microscope was demonstrated. [4] In 1999, CARS microscopy using a collinear geometry and high numerical aperture objective were developed in Xiaoliang Sunney Xie's lab at Harvard University. [5]
In 1978 first theoretical ideas have been developed to break this barrier by using a 4Pi microscope as a confocal laser scanning fluorescence microscope where the light is focused ideally from all sides to a common focus which is used to scan the object by 'point-by-point' excitation combined with 'point-by-point' detection. [9]
STED microscopy is one of several types of super resolution microscopy techniques that have recently been developed to bypass the diffraction limit of light microscopy to increase resolution. STED is a deterministic functional technique that exploits the non-linear response of fluorophores commonly used to label biological samples in order to ...
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