Full text: Technical Commission VIII (B8)

aim is to find fluorescent biosignatures specific to 
cyanobacterial species and crude oil. 
2. MATERIALS AND METHODS 
2.1 Seawater sample preparation 
Seawater samples were collected offshore from Askö Island 
which is located some 80 km south of Stockholm, on 29^ July 
2011. The samples were transported using dry ice and were 
received at UCL on 1% August 2011. Subsequently, these 
samples were stored in a -80 degC freezer until they were 
measured on the 23" August 2011. 
From an optical perspective, natural sea water is comprised of 
three main components: inorganic suspended material, Coloured 
Dissolved Organic Matter (CDOM) and phytoplankton. 
Inorganic suspended material is defined as all inorganic 
particulates that are not included in the phytoplankton 
component CDOM is a group of organic and dissolved 
substances, which consists of humic and fulvic acids. Due to 
their exponential absorption curve with strong absorption from 
UV decreasing towards the red spectral region it is often known 
as yellow substance or ge/bstoff. CDOM has a fluorescence 
peak at an excitation/emission (ex/em) pairing of around 
355/450 nm (Hoge et al, 1993; Nieke et al. 1997) with 
fluorescence efficiency linearly correlated with absorption 
(Green and Blough, 1994). In addition to CDOM, 
photosynthetic pigments of cyanobacterial cells also make a 
significant contribution to the fluorescence emission of 
seawater. Phycocyanin (PC) is a cyanobacteria specific pigment 
receiving and transferring light energy to chlorophyll-a (Chl-a) 
for photosynthetic activity. PC has an absorption peak at 620nm 
with a fluorescence emission peak at 650 nm. Chl-a absorbs 
light at wavelengths of 440 and 680 nm inducing peak 
fluorescence at 685nm. Apart from photosynthetic pigments, 
Nicotinamide Adenine Dinucleotide Phosphate (NADPH) being 
a primary product of photosynthesis, has an absorption peak at 
340 nm and a fluorescence emission peak at 460 nm 
(Steigenberger et al, 2004). In addition to PC and Chl-a 
fluorescence, cyanobacteria also induce fluorescence from the 
aromatic amino acid tryptophan (Dartnell et al., 2010 and see 
Dartnell et al., 2011 for model EEMs and references therein). 
Fluorescence properties of the major constituents of seawater 
are listed in Table 1. 
Prior to the measurements, the seawater samples (frozen after 
sampling for transport) were thawed and centrifuged for 10 
minutes to concentrate the cells present. After resuspending the 
cell pellet, the samples were pipetted into a 3.0 mL quartz 
cuvette and analysed with a Perkin Elmer LS55 Luminescence 
spectrometer (Perkin Elmer, Cambridge, UK) The purpose of 
the centrifuging was to increase the concentration of each 
constituent in the seawater sample and so obtain an improved 
signal to noise ratio. 
2.2 Crude oil sample preparation 
Five different crude oil samples collected from various oil spill 
events were also used for the spectro-fluorescence and optical 
reflectance measurements. All of these oil samples are the 
equivalents of weathered crude oil with diverse consistency in 
terms of their thickness. 
International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, Volume XXXIX-B8, 2012 
XXII ISPRS Congress, 25 August — 01 September 2012, Melbourne, Australia 
To obtain detailed fluorescence features of PAHs, oil samples 
were pipetted into sample well plates and measured with a 
fiber-optic attachment on the same Perkin Elmer LS55 
spectrometer (PE-LS55). 
Before optical reflectance measurements, oil samples were 
transferred onto five black plates, and a Solux light source 
pointed at the samples with a zenith angle of 45 degrees. In the 
mean time, optical fiber probe head was positioned about 3cm 
above the oil samples at a zenith angle of 0 degrees (i.e. nadir- 
viewing angle). The oil sample reflectance was measured using 
an EPP2000 High Resolution spectrometer (Stellarnet, Florida, 
US), and reflectance spectra were recorded from 200 nm up to 
1129 nm. 
2.3 Excitation-emission matrices 
An Excitation-Emission Matrix (EEM) contains entire spectral 
information of measured samples giving a detailed pattern of 
fluorescence intensity of measured samples by covering a broad 
range of both excitation and emission wavelengths (an example 
is given in figure 1). EEMs record a series of emission spectra 
produced by incrementing the excitation wavelengths over a 
broad range of the electromagnetic spectrum from UV to near 
infrared region. It stacks emission spectra generated by the 
excitation into a three-dimensional matrix. Using a contour 
landscape to display and visualise such an information rich 
dataset is an effective means to demonstrate the characterization 
of the fluorescence responding from complex microbial cells 
and other chemical samples. To obtain a clearer visualisation, it 
is reasonable to flatten the 3D landscape into two-dimensional 
planes using colour coding to illustrate the intensity of 
fluorescence emission, so that the emission peaks are not 
obscured behind one another and represents a clear excitation- 
emission map of a sample's fluorescence response (Dartnell et 
al., 2010). 
3. RESULTS 
3.1 Fluorescence properties of cyanobacteria cellular 
pigments 
For the concentrated seawater samples, emission spectra were 
recorded between 300 and 800 nm, with data points logged 
every 0.5 nm. The excitation wavelength was incremented in 15 
nm steps between 240 and 705 nm, and the result of the spectro- 
fluorescence measurements is displayed using EEM in figure 1. 
There are three diagonal intense emission stripes exhibited in 
figure 1. These are artifacts of the spectrometer instrument due 
to diffraction-grating effects of the spectrometer, which is used 
for selecting various excitation wavelengths. To be specific, the 
first diagonal with the steepest gradient on the EEM of 1 is 
caused by Raleigh scattering of the excitation light from 
measured sample. The second and third diagonal strips on the 
EEM with a gradient of 1/2 and 1/3 are second and third order 
harmonic artifacts of excitation light. It is important to know 
that only the emission recorded between the first and second 
diagonal lines is relevant to fluorescence properties of measured 
samples. 
    
   
    
    
     
    
    
   
    
   
  
   
   
    
     
   
   
   
   
   
   
   
    
   
   
   
   
   
    
    
   
   
   
   
    
   
   
    
   
   
   
   
    
      
    
  
   
  
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