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Fluorescent Reference Materials Set
Consists of
six polymer blocks containing seven fluorescent compounds whose
spectra cover a broad spectral range with emission maxima from 330
to 582nm and excitation maxima from 290 to 562 nm. This wide spectral
range enables the user to select a reference material with broadly
similar spectral properties to those of the analyte, ensuring a
reasonable spectral overlap and measurable signals without changing
important parameters such as slit widths and wavlength settings.
Each block
is produced with optically polished surfaces on six sides, with
dimensions of 12.5 x 12.5 x 45mm to fit the standard cell holders
used in spectrofluorimeters. Starna is able to produce these materials
in other sizes and shapes such as rods, cylinders and discs to fit
other instruments and will quote for such requirements. Certain
other materials can also be produced in similar form for specific
studies such as phosphorescence, or singlet and triplet life time
measurements and enquiries are welcome.
Fluorescence
Spectra
Fluorescence
spectra are not absolute in the sense that absorption spectra are
and the appearance of the spectra will depend upon the particular
instrument and the mode used to record it. Most modern instruments
have a choice of operating mode and this needs to be selected according
to the analytical requirement.
Direct measurement
of fluorescent intensity produces very distorted spectra. The effects
of the varying intensity of the source, which falls off considerably
with decreasing wavelength, the sensitivity of the detector which
normally has a maximum in the near UV region and the light throughput
of the monochromators which generally have a maximum in the UV region
and
whose efficiency falls off rapidly at shorter wavelengths and more
gradually at longer wavelengths, are not compensated for. The advantage
of this mode is that as the minimum number of optical components
are used and no signal processing is required, it can produce the
highest sensitivity for quantitative analysis, providing that the
spectra are simple and the bands of interest are well resolved.
The Ratio Mode allows the instrument to monitor the intensity of
the excitation source by means of a reference photomultiplier and
presents the output in terms of a ratio to this reference signal,
thus freeing the recorded spectrum of effects due to the varying
energy of the source. This produces a good signal to noise ratio
and therefore high sensitivity, as well as
monitoring and correcting for drift. For quantitative analysis,
it is usually the mode of choice, particularly for samples which
produce more complex spectra.
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The
Corrected Spectra Mode produces a
spectrum in which many of the above effects are compensated for, usually
by spectral manipulation with a computer, although some older instruments
may still use electo-optical methods to achieve the adjustments. This
mode produces an excitation spectrum which has similar characteristics
to that of the UV-Visible absorption spectrum. The sensitivity of
the fluorescence spectra is much higher than that of the absorption
spectrum, but direct comparisons can still be made, as the shapes
are similar. It is also possible to make quantum yield
measurements and energy yield calculations from the corrected spectra.
This feature may be ofassistance if the instrument is being used to
assist with the identification of the analyte, as these properties
are known for a large number of substances. This mode also permits
the comparison of data from different instruments which should show
similar wavelengths for excitation maxima and minima, as well as similar
values for ratios of the intensity of different bands and similar
shapes for the spectral bands. Such spectra are particularly useful
for publication and inter-laboratory studies, as uncorrected spectra,
even those run on
similar types of instrument, will include the various distortions
introduced by the particular apparatus.
Wavelength
Calibration
The spectra of the materials provided in this set of
reference materials are well established and their maxima and minima
may be used to check the wavelength calibration of instruments which
operate with narrow spectral band widths. Materials which produce
narrow bands, such as anthracene and ovalene are particularly suitable
for this application. However, it is important to ensure that such
calibrations are carried out in the corrected mode at small spectral
bandwidths, or errors can be introduced by peak broadening or apparent
wavelength shifts due to instrumental effects.
The illustrated spectra were obtained
using a Perkin Elmer LS50B spectrofluorimeter and the spectral band
widths 2.5nm for all spectra. These spectra are for guidance only
and will vary in shape if different spectral band widths are used.
The peak wave lengths are only comparable for instruments operating
in the corrected spectra mode. If this mode is not available, it
is important that all instrument settings are reproduced exactly
on each occasion, in order to ensure that subsequent comparisons
are valid.
Selectivity
Molecular Fluorescence Spectrometry is a more selective
technique than UV-Visible Spectrophotometry. Material No.1 contains
a mixture of Anthracene and Naphthalene and may be used to demonstrate
the greater selectivity of the fluorescence technique. By exciting
at two different wave lengths, the emission spectrum of either substance
can be obtained free of interference from the other.
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