STRUCTURAL
MAGNETISM, TOOL OF TECTONIC ANALYSIS AT DIFFERENT SCALES (FROM
OUTCROP TO REGIONAL) :
EXAMPLES FROM CORBIERES,
FRANCE.
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defended on the 20th of September 2002
in front of a jury composed of : |
MM. |
Martin BURKHARD, |
Professor at the University of Neuchâtel
(Switzerland) President |
Dominique FRIZON de LAMOTTE, |
Professor at the UCP Supervisor |
Philippe ROBION, |
Maître de Conférence at the UCP Co-Supervisor |
Jean-Luc BOUCHEZ, |
Professor at the Univ. of Toulouse Rapporteur |
Jean-Christophe MAURIN, |
Professor at the Univ. of La Rochelle Rapporteur |
Catherine KISSEL, |
Research ingenior at the LSCE (CEA-CNRS) Gif-sur-Yvette Examiner |
Bernard HENRY, |
Research director, IPG Invited |
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Anisotropy
of magnetic susceptibility (AMS) is commonly used to define shortening
directions because AMS is efficient even if strain is to weak to be
macroscopically visible. We focus here on the ASM answer to polyphased
strain, either
linked to two distinct and successive shortening directions, or to
succession of layer parallel shortening (LPS) and folding. In this way,
a sampling
has been performed in the Pyrenean foreland in different structural
positions of the Lagrasse fold (Corbières, France) and in the different
sheets of the “La Cagalière” duplex, hectometric
structure in the depths of the Lagrasse fold. All these structures
were emplaced
in two successive shortening directions.
While regionally recorded AMS is early tectonic anisotropy connected to
LPS in the first direction, is not altered by the second one and is only
sheared during folding, AMS is really different close to thrusts and without
any simple meaning at first sight. The use of a thermic treatment on these
sites allowed us to decipher the early tectonic anisotropy due to LPS and
thus to rediscover informations about the first shortening direction underwent
and rotations about vertical axis recorded since then. This early anisotropy
is thus not erased but only masked by later crystallizations, and this
technique turn out to be valid in different facies. By return, those data
allowed us to interpret the duplex as a stopping structure of the lateral
propagation of the Lagrasse fold thrust, and to chronogically place the
duplex emplacement between this stopping and the sliping transfer on an
out-of-sequence thrust.
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