4
Outstanding Simplicity of Operation
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The RF-1501 uses blazed holographic, concave gratings, a non-
spherical condenser lens, and the latest digital signal processing
circuit, to provide exceptionally high sensitivity, expected only with
a more expensive instrument. The signal-to-noise ratio for the
Raman lines of distilled water is higher than 300.
Scanning speed is selectable in 4 steps, with superfast
wavelength collection at 3,700 nm/min. The spectrum of
anthracene shown to the right, for example, is obtained in about 3
seconds. And, wavelength slewing is possible at ultrahigh speed
of about 30,000 nm/min. (500 nm/sec.). This allows wavelength
to be set to the desired point in an instant.
The search function enables automatic detection of the optimal
excitation and emission wavelengths for your sample, by
automatically distinguishing the emission light from the scattered
excitation light, Raman scattered light, and secondary light.
Exceptionally High Sensitivity
High Speed
Automatic Search of Optimal Wavelengths
Scattered excitation light
Scattered Roman light of solvent
Fluorescence of sample
Secondary light of
scattered light
Wavelength
Fluorescence
of impurities
in sample
Fluorescence intensity
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