Ductile deformation within Upper Himalaya Crystalline Sequence and geological implications, in Nyalam area, Southern Tibet.
LIU XiaoBing 1,2,3*, LIU XiaoHan 1, LELOUP P. H. 2, MAHEO G. 2, PAQUETTE J. L. 4, ZHANG XinGang 3 & ZHOU XueJun 1
1
Key Laboratory of Continental Collision and Plateau Uplift, Institute
of Tibetan Plateau Research, Chinese Academy of Sciences, Beijing
100085, China;
2 Laboratoire des sciences de la terre de Lyon,
Terre, Planètes, Environement, CNRS UMR 5276, Université Lyon1 – ENS
Lyon, Villeurbanne, 69622, France;
3 Graduate University of Chinese Academy of Sciences, Beijing 100049, China;
4 Laboratoire Magmas et Volcans, CNRS UMR 6524, Université Blaise Pascal, Clermont-Ferrand, 63038, France
Abstract
The
South Tibet Detachment System (STDS) is a flat normal fault that
separates the Upper Himalaya Crystalline Sequence (UHCS) below from the
Tethyan Sedimentary Sequence (TSS) above. Timing of deformations
related to the STDS is critical to understand the mechanism and
evolution of the Himalaya collision zone. The Nyalam detachment (ND)
(~86°E) locates in the middle portion of STDS (81°–89°E). Dating of
deformed leucocratic dykes that are most probably syntectonic at
different depth beneath the ND, allow us to constrain the timing of
deformation. (1) Dyke T11N37 located ~3500 m structurally below the ND
emplaced at 27.4±0.2 Ma; (2) Dyke T11N32 located ~1400 m structurally
below the ND emplaced at 22.0±0.3 Ma; (3) T11N25 located within the top
to the north STD shear zone, ~150 m structurally below the ND, emplaced
at 17.1±0.2 Ma. Combining ND footwall cooling history and T11N25
deformation temperature, we indicate a probable onset of top to the
north deformation at ~16 Ma at this location.
These results show an
upward younging of the probable timing of onset of the deformation at
different structural distance below the ND. We then propose a new model
for deformation migration below the ND with deformation starting by
pure shear
deformation at depth prior to ~27.5 Ma that migrates
upward at a rate of ~ 0.3 mm/a until ~18 Ma when deformation switches
to top to the north shearing in the South Tibet Detachment shear zone
(STDsz). As deformation on the ND stops at 14–13 Ma this would imply
that significant top to the North motion would be limited to less than
5 Ma and would jeopardize the importance of lower channel flow.
Chin Sci Bull, doi: 10.1007/s11434-012-5228-6