Ultra-sensitive optical oxygen sensors for characterization of nearly anoxic systems
Oxygen quantification
in trace amounts is essential in many fields of science and technology. Optical oxygen sensors proved invaluable tools for oxygen measurements in a broad
concentration range, but until now neither optical nor electrochemical oxygen
sensors were able to quantify oxygen
in the sub-nanomolar concentration range. Herein we present new optical
oxygen-sensing materials with unmatched sensitivity. They rely on the
combination of ultra-long decaying (several 100 ms lifetime) phosphorescent
boron- and aluminium-chelates, and highly oxygen-permeable and chemically stable
perfluorinated polymers. The sensitivity of the new sensors is improved up to
20-fold compared with state-of-the-art analogues. The limits of detection are
as low as 5 p.p.b., volume in gas phase under atmospheric pressure or 7 pM in
solution. The sensors enable completely new applications for monitoring of oxygen in previously inaccessible
concentration ranges.
Oxygen undoubtedly belongs to the most important analytes on
earth. Traditionally, most oxygen sensors were designed for the physiological
range. However, numerous applications require monitoring of oxygen at significantly lower
concentrations, for example, corrosion protection,
surface treatment, the semiconductor industry and biological research. For
instance, it was demonstrated that bacteria can show respiration and
potentially aerobic growth far below the Pasteur point (~10 μM dissolved oxygen (DO)). Recently, sensors that
quantify DO in concentration ranges of 100 nM and below have gained special
interest as biologists explore aerobic life in areas very close to anoxic
conditions. Unfortunately, few sensors are capable to resolve at such low
concentration, and measurements below 0.5 nM are currently impossible.
Optical sensors
proved to be indispensable tools for oxygen
quantification that have mostly replaced the more conventional Clark electrode. Their advantages include minimal
invasiveness, simplicity, suitability for miniaturization, versatility of
formats (planar optodes, fibre-optic sensors, micro- and nanoparticles, paints
and so on) and suitability for imaging of oxygen distribution on surfaces or in
volume. Moreover, optical oxygen sensors are tuneable over a wide range of
concentrations. Optical oxygen sensors rely on quenching of a phosphorescent
indicator by the analyte. Both the nature of the indicator and the matrix
(which acts as a solvent and support for the dye and as a permeation-selective
barrier) are of great importance since the sensitivity of an oxygen sensor is
roughly proportional to the luminescence decay time of the indicator and to the
oxygen permeability of the matrix.
State-of-the-art indicators are dominated by phosphorescent complexes with
platinum group metals that possess decay times varying from microseconds to a
few milliseconds. Dyes with significantly longer decay times are extremely rare
and are so far limited to fullerenes(which have rather low luminescence
brightness at ambient temperatures) and some phosphorescent BF2-chelates.
Both classes are not inherently compatible with highly oxygen-permeable matrices (for example,
silicone and Teflon AF). Hence, the sensors based on these indicators and other
matrices (for example, ethylcellulose and polystyrene (PS)) are not drastically
more sensitive than sensors relying on more conventional dyes (for example,
Pd(II) porphyrins) immobilized in highly oxygen-permeable
polymers.
Herein, we
present a new type of oxygen-sensing materials that show sensitivities well
beyond state-of-the-art trace oxygen sensors. They rely on new blue
light-excitable BF2 and Al(III) chelates featuring ultra-long room
temperature phosphorescence. The chelates are modified with perfluoroalkyl
chains to ensure compatibility with highly oxygen-permeable and chemically inert
perfluorinated polymers. The resulted ultra-sensitive sensors are ideally
suitable for characterization of nearly anoxic systems.
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