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Technical
Information: RazorEdge® Filter Layouts |
| Filters play a crucial role in enabling high-fidelity Raman spectroscopy measurements. In many simple laboratory layouts the only filters needed are a laser-transmitting filter to clean-up the laser spectral output and a laser-blocking filter to ensure that no Rayleigh-scattered laser light reaches the detection system (see Filter Types for Raman Spectroscopy Applications). However, in many high-performance Raman systems – such as those with microscopic imaging capabilities or highly sensitive remote probes – expensive and/or complex focusing and collection optics are used to couple the system to the sample region. For these systems it is desirable for the excitation laser beam and the Raman-shifted signal light to share a common light path. The illustrations below show how this layout can be accomplished with an ultrasteep dichroic beamsplitter used in conjunction with a laser-blocking filter. Semrock's RazorEdge Dichroic™ beamsplitter filters are ideal for these applications. |
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In the
standard Raman spectroscopy layout, the laser excites the sample
directly, and a laser-blocking filter (such as the ultrasteep RazorEdge
filter) is positioned between the sample and the spectrometer with light
incident at or near normal incidence – its job is to block the scattered
laser light and pass the Raman-shifted signal light as close as possible
to the laser wavelength and with as much transmission as possible. RazorEdge
filters are ideal for this configuration. |
In focusing
or imaging systems that utilize high-NA collection optics, for example,
it is convenient for the incident laser beam and collected signal light
to share a common path. To meet this requirement, a two-filter solution
is ideal: a 45° beamsplitter reflects the laser light and directs
it through the optics to the sample, while efficiently transmitting the
returning Raman-shifted signal light; a laser-blocking filter at normal
incidence is used in conjunction with the beamsplitter to completely block
the undesired laser light from the spectrometer. |
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| In order for the two-filter configuration shown above right to work, the 45° beamsplitter must be as steep as the laser-blocking filter. Traditionally thin-film filters could not achieve very steep edges at 45° because of the "polarization splitting" problem – the edge position tends to be different for different polarizations of light. However, through continued innovation in thin-film filter technology, Semrock has been able to achieve ultrasteep 45° beamsplitters with the same steepness of our renowned RazorEdge laser-blocking filters: the transition from the laser line to the passband of the filter is guaranteed to be less than 1% of the laser wavelength (for U-grade filters)! |
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