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@ARTICLE{Bohn:828469,
author = {Bohn, Birger and Lohse, Insa},
title = {{C}alibration and evaluation of {CCD} spectroradiometers
for airborne measurements of spectral actinic flux
densities},
journal = {Atmospheric measurement techniques discussions},
volume = {},
issn = {1867-8610},
address = {Katlenburg-Lindau},
publisher = {Copernicus},
reportid = {FZJ-2017-02428},
pages = {1 - 31},
year = {2017},
abstract = {The properties and performance of CCD array
spectroradiometers for the measurement of atmospheric
spectral actinic flux densities and photolysis frequencies
were investigated. These instruments are widely used in
atmospheric research and are suitable for aircraft
applications because of high time resolutions and high
sensitivities in the UV range. The laboratory
characterization included instrument-specific properties
like wavelength accuracy, dark signals, dark noise and
signal-to-noise ratios. Spectral sensitivities were derived
from measurements with spectral irradiance standards. The
calibration procedure is described in detail and a
straightforward method to minimize the influence of stray
light on spectral sensitivities is introduced. Detection
limits around 1×1010cm−2 s−1 nm−1 were derived for
spectral actinic flux densities in a 300 nm range (1 s
integration time). As a prerequisite for the determination
of stray light under field conditions, atmospheric cutoff
wavelengths were defined using radiative transfer
calculations as a function of solar zenith angles and ozone
columns. The recommended analysis of field data relies on
these cutoff wavelengths and is also described in detail
taking data from a research flight as an example. An
evaluation of field data was performed by ground-based
comparisons with a double-monochromator reference
spectroradiometer. Spectral actinic flux densities were
compared as well as photolysis frequencies j(NO2) and
j(O1D), representing UV-A and UV-B ranges, respectively. The
spectra expectedly revealed an increased daytime level of
residual noise below atmospheric cutoff wavelengths that is
caused by stray light. The influence of instrument noise and
stray light induced noise was found to be insignificant for
j(NO2) and rather limited for j(O1D), resulting in estimated
detection limits of 5×10−7 s−1 and 1×10−7 s−1,
respectively. For j(O1D) the detection limit could be
further reduced by setting spectral actinic flux densities
below cutoff wavelengths to zero. The accuracies of
photolysis frequencies were determined from linear
regressions with reference instrument data. The agreement
was typically within ±5 $\%.$ Optical receiver aspects were
widely excluded in this work and will be treated in a
separate paper in particular with regard to airborne
applications. Overall, the investigated instruments are
clearly suitable for high quality photolysis frequency
measurements with high time resolution as required for
airborne applications. An example of data from a flight on
the research aircraft HALO is presented.},
cin = {IEK-8},
ddc = {550},
cid = {I:(DE-Juel1)IEK-8-20101013},
pnm = {243 - Tropospheric trace substances and their
transformation processes (POF3-243)},
pid = {G:(DE-HGF)POF3-243},
typ = {PUB:(DE-HGF)16},
doi = {10.5194/amt-2017-74},
url = {https://juser.fz-juelich.de/record/828469},
}