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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

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