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100 L. BARATOUX ETAL.regime but under different thermal conditions(Stfpsk~i et al. 2001).Methods <strong>and</strong> techniquesMineral chemistryMinerals were analysed with a Cameca SX 100electron microprobe equipped with four WDSspectrometers at Blaize Pascal University,Clermont-Ferr<strong>and</strong>, France. Operating conditionswere 15kV, 10hA beam current, 2-5p~mbeam diameter, 20 s counting time, <strong>and</strong> naturalmineral st<strong>and</strong>ards. Some hornblende <strong>and</strong> plagioclasewere analysed using a CamScan $4scanning electron microscope <strong>and</strong> attachedLink EDX microanalytical system, at CharlesUniversity, Prague, Czech Republic. Operatingconditions were 20 kV, 1.8 nA beam current,1-3 p,m beam diameter, 120 s counting time,<strong>and</strong> mineral st<strong>and</strong>ards Structure Probe Instruments(SPI). Ca maps from plagioclase weremade at Claude Bernard University in Lyon,with operating conditions 15 kV, 15 nA beamcurrent <strong>and</strong> spatial resolution <strong>of</strong> 512 x 512pixels.<strong>Quantitative</strong> micro<strong>structural</strong> analysis<strong>Quantitative</strong> micro<strong>structural</strong> analysis <strong>of</strong> grainboundaries was carried out on traced <strong>and</strong> digitizedoutlines <strong>of</strong> grains in ESRI ArcView 3.2Desktop GIS environment. The map <strong>of</strong> grainboundaries was generated using ArcView extensionPoly (Lexa 2003). The resulting polygonshave been treated by MATLAB TM PolyLXToolbox (http://petrol.natur.cuni.cz/~ ondro;Lexa 2003), in which grain shape <strong>and</strong> grainboundary preferred orientations (SPO <strong>and</strong>GBPO, respectively) were analysed using themoments <strong>of</strong> inertia ellipse fitting <strong>and</strong> eigenanalysis<strong>of</strong> bulk orientation tensor techniques (Lexa,2003; modified SURFOR technique by Panozzo(1983) for GBPO). Their degree is expressed asthe eigenvalue ratio (r = E1/E2) <strong>of</strong> the weightedorientation tensor <strong>of</strong> grain shapes or boundaries.The orientation is defined by V~ <strong>and</strong> V2 eigenvectors.The grain sizes <strong>of</strong> the minerals werecalculated in terms <strong>of</strong> Ferret diameters <strong>of</strong> grainsection without stereological corrections.Crystallographic preferred orientationAmphibole <strong>and</strong> plagioclase crystallographic preferredorientations (CPO) were collected using ascanning electron microscope CamScan $4 inPrague <strong>and</strong> a JEOL JSM 5600 in Montpellierequipped with Channel5 electron backscatterdiffraction (EBSD) system from HKL Technology(Prior et al. 1999). Thin sections werepolished using 0.25 ~m diamond paste. Toremove all surface damage <strong>and</strong> minimize reliefbetween minerals, sections were chemicallypolished using a colloidal silica suspension. Allthin sections were carbon-coated. The coatingreduces the quality <strong>of</strong> the electron backscatterdiffraction patterns (EBSP) so that automaticindexing mode <strong>of</strong> the EBSP system could notbe used. Most data were therefore collectedmanually. Operating conditions were 20 kV inPrague <strong>and</strong> 15 kV in Montpellier, 5.6 nA beamcurrent, working distance 39 ram, <strong>and</strong> 2-5 ~mbeam diameter. For each measurement, threeEuler angles (vl, 05, v2) characterizing thelattice orientation as well as the nature <strong>of</strong> themineral were determined <strong>and</strong> stored. Practiceshows that plagioclase diffraction patterns donot change significantly from albite up to atleast An65 (Lapworth et al. 2002). Therefore,the Anorthite48 database was used for indexingplagioclase. Pole figures <strong>and</strong> inverse polefigures were projected using the s<strong>of</strong>tware developedby D. Mainprice (ftp://ftp.dstu.univmontp2.fr/pub/TPHY/david/pc).Projections<strong>of</strong> crystallographic axes ([a], [b] <strong>and</strong> [c]) oroptical indicatrix (o~, /3, <strong>and</strong> 3/) are generallyused for plagioclase (e.g. Jensen & Starkey1985; Olsen & Kohlstedt 1985; Ji & Mainprice1988, 1990; Prior & Wheeler 1999).The degree <strong>of</strong> CPO has been quantified usingorientation tensor <strong>of</strong> crystallographic planes<strong>and</strong> directions (Mainprice, ftp://ftp.dstu.univmontp2.fr/pub.TPHY/david/pc).The intensity<strong>of</strong> CPO is given by the I parameter (Lisle 1985):3I = 15/2 x Z(Ei - 1/3) 2i=1where E~, E2, <strong>and</strong> E3 represent the eigenvalues <strong>of</strong>the preferred orientation <strong>of</strong> poles to planes <strong>and</strong>directions <strong>of</strong> amphibole <strong>and</strong> plagioclase grainsplotted in pole figures. The values <strong>of</strong> I rangebetween 0 (no preferred orientation) <strong>and</strong> 5 (allfabric elements perfectly parallel one to another).MicrostructuresThe metagabbros from the eastern (lower) beltare affected by localized shear zones (Fig. lb)<strong>and</strong> all stages from non-deformed rock, protomylonite,mylonite, <strong>and</strong> up to highly strainedultramylonite are present (Figs 2a, b, c <strong>and</strong> d).In the western metagabbro (upper) belt, theprotolith stage is not preserved <strong>and</strong> only twodeformational stages can be distinguished252

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