Priscille Lesne
University of Bristol
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Featured researches published by Priscille Lesne.
Journal of Petrology | 2018
Michel Pichavant; Stéphane Poussineau; Priscille Lesne; C Solaro; Jean-Louis Bourdier
New petrological data on eruption products and experimental results are integrated and a model for the evolution of the La Soufriere (Guadeloupe, Lesser Antilles arc) magma reservoir prior to the 1530 AD eruption is presented. In comparison with recent volcanic crises in the Antilles, the 1530 AD eruption is distinctive. The eruptive pyroclastic sequence shows a continuous zonation in whole-rock composition from silicic (∼ 62 wt% SiO2) to mafic andesite (∼ 55 wt% SiO2). Mafic products are estimated to be 80% of the total eruption volume. All juvenile clasts are crystal-rich (46-60 vol.% phenocrysts), the crystallinity being inversely correlated with the bulk-rock SiO2 content. The phenocryst assemblage (plagioclase, orthopyroxene, clinopyroxene, magnetite) is constant throughout the sequence. Complexly zoned crystals are encountered, but An60-65, En56-59 and Mt66-68 compositions occur in all samples. Glass inclusions are rhyolitic with up to 5-5.5 wt % H2O. Matrix glasses are strongly heterogeneous, from ∼64 to > 76 wt % SiO2. The pre-eruptive evolution of the reservoir is dominated by the remobilization of a resident andesitic body following the arrival of a basaltic magma batch. Conditions of early remobilization are constrained from experiments on a basalt from the L’Echelle scoria cone. The arrival magma is a crystal-poor, moderately hot (975-1025 °C), wet (> 5 wt % H2O) and oxidized (NNO+1) low-MgO high alumina basalt similar to those involved in other Antilles volcanic centers. Geothermometry and experiments on a silicic andesite product of the eruption show that, for melt H2O contents between 5 and 5.5 wt %, phenocrysts and interstitial melt in the resident magma were in mutual equilibrium at ∼875 °C and NNO+0.8. However, matrix glass and glass inclusion compositions show that, locally, the andesite body was as cold as 825 °C. Melt volatile concentrations imply a minimum depth for the magma reservoir between 5.6 and 7.1 km, and the absence of amphibole phenocrysts indicates a maximum depth at 8.5 km. The 1530 AD eruption tapped an hybrid magma assembled by mixing approximately equal proportions of resident andesite and arrival basalt. Mineralogical indicators of the mixing event include An-rich layers in plagioclase, En-rich rims on orthopyroxene and core-rim zonation in magnetite, but overall phenocrysts were little modified during assembly of the hybrid magma. In comparison, matrix glasses were more severely affected. Mixing proceeded essentially by the addition of a mafic melt to the andesite body. The continuous chemical zonation observed in 1530 AD eruption products reflects mixing between three components (mafic melt, silicic melt, phenocryst assemblage). Timescales measured on different eruptive products range from several thousand years (U-Th-Ra disequilibria), 10s days (diffusion modelling in orthopyroxenes) to 10s hours (heterogeneous matrix glasses). Short timescales since mafic recharge, lack of extensive transformations of phenocrysts, continuous whole-rock chemical zonation and predominance of mafic products are all consistent with triggering of the 1530 AD eruption by a major mafic recharge event which originated in the middle to lower Lesser Antilles arc crust.
American Mineralogist | 2017
Yann Morizet; Emanuela Gennaro; Sébastien Jego; Zoltán Zajacz; Giada Iacono-Marziano; Michel Pichavant; Ida Di Carlo; Clément Ferraina; Priscille Lesne
Abstract Sulfur is an important volatile element involved in magmatic systems. Its quantification in silicate glasses relies on state-of-the-art techniques such as electronprobe microanalyses (EPMA) or X-ray absorption spectroscopy but is often complicated by the fact that S dissolved in silicate glasses can adopt several oxidation states (S6+ for sulfates or S2− for sulfides). In the present work, we use micro-Raman spectroscopy on a series of silicate glasses to quantify the S content. The database is constituted by 47 silicate glasses of various compositions (natural and synthetic) with S content ranging from 1179 to 13 180 ppm. Most of the investigated glasses have been synthesized at high pressure and high temperature and under fully oxidizing conditions. The obtained Raman spectra are consistent with these fO2 conditions and only S6+ is present and shows a characteristic peak located at ~1000 cm−1 corresponding to the symmetric stretch of the sulfate molecular group (ν1 SO42−
Journal of Petrology | 2011
Priscille Lesne; Simon C. Kohn; Jon D Blundy; Fred Witham; Roman E. Botcharnikov; Harald Behrens
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Computers & Geosciences | 2012
Fred Witham; Jonathan D. Blundy; Simon C. Kohn; Priscille Lesne; Jacqueline Dixon; Sergey V. Churakov; Roman E. Botcharnikov
). The intensity of the ν1 SO42−
Contributions to Mineralogy and Petrology | 2011
Priscille Lesne; Bruno Scaillet; Michel Pichavant; Giada Iacono-Marziano; Jean-Michel Bény
\begin{array}{} \text{SO}_4^{2-} \end{array}
Geochimica et Cosmochimica Acta | 2009
Maxime Mercier; Andrea Di Muro; Daniele Giordano; Nicole Métrich; Priscille Lesne; Michel Pichavant; Bruno Scaillet; Roberto Clocchiatti; Gilles Montagnac
peak is linearly correlated to the parts per million of S6+ determined by EPMA. Using subsequent deconvolution of the Raman spectra, we established an equation using the ratio between the areas of the ν1 SO42−
Contributions to Mineralogy and Petrology | 2011
Priscille Lesne; Bruno Scaillet; Michel Pichavant; Jean-Michel Bény
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Chemical Geology | 2015
Priscille Lesne; Bruno Scaillet; Michel Pichavant
peak and the silicate network species (Qn) in the high-frequency region: ppm S6+=34371ASO42−AQn±609.
Archive | 2017
Yann Morizet; Emanuela Gennaro; Sébastien Jégo; Zoltán Zajacz; Giada Iacono-Marziano; Michel Pichavant; Ida Di Carlo; Clément Ferraina; Priscille Lesne
Archive | 2010
Priscille Lesne; Simon C. Kohn; Jonathan D. Blundy; Fred Witham; Roman E. Botcharnikov; Harald Behrens
\begin{array}{} \text{ppm S}^{6+}=34371\frac{A\text{SO}_4^{2-}}{A\text Q^{\text n}}\pm609. \end{array}