Barletta et al 2010.pdf - Department of Geological Sciences ...
Barletta et al 2010.pdf - Department of Geological Sciences ...
Barletta et al 2010.pdf - Department of Geological Sciences ...
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2318<br />
F. <strong>Barl<strong>et</strong>ta</strong> <strong>et</strong> <strong>al</strong>. / Quaternary Science Reviews 29 (2010) 2315e2324<br />
Fig. 3. (A) Representative hysteresis loops (left diagrams) with the corresponding IRM acquisition curves (right diagrams). The hysteresis param<strong>et</strong>ers (saturation magn<strong>et</strong>ization<br />
(M S ), saturation remanence (M R ) and coercivity (H C )) were d<strong>et</strong>ermined from the paramagn<strong>et</strong>ic-corrected hysteresis data (broken curve in the left diagrams). Vertic<strong>al</strong> line at 100 mT<br />
is for reference.<br />
v<strong>al</strong>ue) using the s<strong>of</strong>tware developed by Mazaud (2005). These three<br />
param<strong>et</strong>ers are useful to characterize the mean coercivity state <strong>of</strong><br />
the ferrimagn<strong>et</strong>ic miner<strong>al</strong>s which in turn depends on both the<br />
magn<strong>et</strong>ic miner<strong>al</strong>ogy and grain size (e.g., Dunlop and Özdemir,<br />
1997). Furthermore, the magn<strong>et</strong>ic grain size was estimated using<br />
k ARM versus k LF diagram (King <strong>et</strong> <strong>al</strong>., 1983). The objective here is not<br />
to d<strong>et</strong>ermine the absolute size <strong>of</strong> the magn<strong>et</strong>ic grains as it was<br />
previously shown that ARM measurements vary from one laboratory<br />
to the other (Sagnotti <strong>et</strong> <strong>al</strong>., 2003), but rather to assess the<br />
extent and uniformity <strong>of</strong> the magn<strong>et</strong>ic grain size distribution.<br />
Fin<strong>al</strong>ly, a sm<strong>al</strong>l quantity <strong>of</strong> sediment was collected every 10 cm over<br />
the top 3 m and in some selected interv<strong>al</strong>s in order to study both<br />
the hysteresis properties and the IRM acquisition curves using an<br />
<strong>al</strong>ternating gradient force magn<strong>et</strong>om<strong>et</strong>er (AGM) (Princ<strong>et</strong>on<br />
Measurement Corporation model MicroMag 2900 AGM) at the<br />
P<strong>al</strong>eomagn<strong>et</strong>ism laboratory <strong>of</strong> the Institut des sciences de la mer de<br />
Rimouski (ISMER).<br />
3.2. Computerized axi<strong>al</strong> tomography an<strong>al</strong>ysis (CAT-scan)<br />
Digit<strong>al</strong> X-ray images <strong>of</strong> <strong>al</strong>l u-channel samples were obtained by<br />
computerized axi<strong>al</strong> tomography (CAT-scan) an<strong>al</strong>ysis with a 1-mm<br />
downcore resolution. The resulting gray sc<strong>al</strong>e images <strong>al</strong>low us to<br />
extract a tomographic intensity pr<strong>of</strong>ile (CT numbers; e.g., St-Onge<br />
<strong>et</strong> <strong>al</strong>., 2007). CT numbers primarily reflect changes in sediment<br />
bulk density, miner<strong>al</strong>ogy as well as porosity and can be <strong>al</strong>so useful<br />
to d<strong>et</strong>ect core deformation or coring artefacts (e.g., Guyard <strong>et</strong> <strong>al</strong>.,<br />
2007; St-Onge <strong>et</strong> <strong>al</strong>., 2007).<br />
3.3. Grain size an<strong>al</strong>yses<br />
Grain size measurements on Core 650 were made using<br />
a Beckman-Coulter laser diffraction an<strong>al</strong>yzer (Model LS-13320;<br />
0.04e2000 mm) at ISMER at 10 cm interv<strong>al</strong>s. About 0.5 g <strong>of</strong> w<strong>et</strong><br />
sediment was mixed in C<strong>al</strong>gon electrolytic solution (sodium