The South Tibet Detachment shear zone in the Dinggye area. Time constraints on extrusion models of the Himalayas.
P.H. Leloup (1); G. Mahéo (1); N. Arnaud (2); E. Kali (3); E. Boutonnet (1); Dunyi Liu (4); Liu Xiaohan (5); Li Haibing (4).
(1) CNRS UMR 5570 Université Lyon1 - ENS Lyon, Villeurbanne, France.
(2) Géosciences Montpellier, Université de Montpellier2, Montpellier France.
(3) Institut de Physique du Globe de Strasbourg (CNRS, UdS/EOST), UMR 7516, Strasbourg, France.
(4) Laboratory of Continental Dynamics, Institute of Geology, CAGS, Beijing, China
(5) Institute of Tibetan Plateau Research, Chinese Academy of Sciences, Beijing, China
Abstract
We
investigate the timing of end of motion along the South Tibet
detachment system (STDS), a major normal fault system that runs
parallel to the Himalayan range for more than 1500km. Near Dinggye (~
28°10’N, 87°40’E), the STD dips ~10±5° to the North and separates
Paleozoic Tethyan series from Upper Himalayan Crystalline Series
(UHCS). Immediately below the STD, the UHCS is highly deformed in the
STD shear zone, lineations trend NNE and the shear senses are top to
the NE. In micaschist, P-T path constrained by pseudosection and garnet
chemistry, shows successive metamorphic conditions of ~0.6 GPa and
~550°C and 0.5 GPa and 625°C. U/Pb dating of Monazite and zircons in
deformed and undeformed leucogranites suggest that ductiledeformation
lasted until at least ~16 Ma but ended prior to ~15Ma in the STD shear
zone ~100 meters below the detachment. Ar/Ar micas ages in the footwall
span between ~14.6 and 13.6 Ma, indicating rapid cooling down to
~320°C, and suggesting persistence of normal faulting, at that time.
The STDS is cut and offset by the N-S trending Dinggye active normal
fault which initiated prior to 11Ma thus providing a minimum bound for
the end of STDS motion. These data are interpreted as reflecting 0.3
GPa (11km) to 0.6 GPa (22km) of exhumation along the STDS starting
prior to ~16 Ma, ending between 13.6 and 11 Ma. The 1000 km long
stretch of the STDS east of the Gurla Mandata probably stopped almost
synchronously between 13 and 11 Ma ago, coevally with a sudden switch
from NNE-SSW to E-W extension at the top of the accretionary prism,
with jump of the major thrust from the lower Main Central Thrust (MCTl)
to the Main the Boundary Thrust (MBT), and with change in India and
Asia convergence direction. This synchronism is probably better explain
in the frame of a thrust wedge or thrust system model than a lower
channel flow model. West of the Gurla Mandata the STDS appears to stop
5 to 3 Ma earlier, possibly related to local interactions with the
Karakorum fault in a way that needs to be understand.
E.P.S.L. 292, p. 1–16, 2010.