Tectonophysics [T]

T32C
 MC:3003  Wednesday  1020h

Exhumation of High- and Ultrahigh-Pressure Rocks: The Cross-Disciplinary View I


Presiding:  C Warren, Earth and Environmental Sciences, The Open University; D Young, Department of Geological Sciences, University of Texas at San Antonio; E Peterman, Department of Earth Science, University of California at Santa Barbara

T32C-01 INVITED

Testing exhumation models – the roles of field data and of dating structures

* Wheeler, J johnwh@liv.ac.uk, University of Liverpool, Dept. Earth and Ocean Sciences, Liverpool, L69 3GP, United Kingdom

What distinguishes different models for HP/UHP exhumation, and how may they be tested? All models for exhumation involve the relative movements of bodies of rock. The dynamics – the driving force – for exhumation has often been given prominence in the description of exhumation models over the past 20 years. However the driving force – or the past distribution of stress during exhumation – is almost impossible to constrain by observation. There is instead much more scope for constraining the kinematics. Structures and kinematic indicators can give relative movements. Such structures can be dated directly, or dated indirectly by comparing PTt paths around them. It is instructive, then, to compare different exhumation models with reference to their kinematic implications. Many interpretations now involve thrusting below an HP/UHP unit (or "sliver"), with "normal sense" faulting or ductile shear above it but with the opposite movement sense. Consequently the HP/UHP unit moves up relative to rocks both above and below it. This has been proven for example in the Alps. It is important to note that proof of such a mechanism must involve dating both the normal sense movement and the thrusting – it is not sufficient to just deploy movement sense, because the ages might be different. The kinematics of this model are the same as for "channel flow" as invoked in the Himalayas. Apart from the fact the exhumed core region is not HP in the Himalayas, are there criteria that, objectively, distinguish the two models? I have asserted that the Alpine exhumation was driven by buoyancy of the exhumed material, plausible if it was buried below a dense mantle wedge. Channel flow is driven by a push from behind and squeezing. I will discuss whether the overall size and internal strain of bodies of exhumed material could be used to distinguish different driving forces.

T32C-02 INVITED

Exhumation of the Ultrahigh-Pressure Western Gneiss Region: Structural Geology, Petrology and Geochronology

* Hacker, B hacker@geol.ucsb.edu, Earth Science, University of California, Santa Barbara, CA 93106,
Andersen, T B t.b.andersen@geologi.uio.no, Geosciences, Universitetet i Oslo, Oslo, 0316, Norway
Barth, N ncbarth@umail.ucsb.edu, Earth Science, University of California, Santa Barbara, CA 93106,
Johnston, S scojoh@email.arizona.edu, Physics, California Polytechnic State University, San Luis Obispo, CA 93407,
Kylander-Clark, A R akylander@umail.ucsb.edu, Earth Science, University of California, Santa Barbara, CA 93106,
Peterman, E epeterman@umail.ucsb.edu, Earth Science, University of California, Santa Barbara, CA 93106,
Walsh, E ewalsh@cornellcollege.edu, Geology, Cornell College, Mount Vernon, IA 52314,
Young, D David.Young@utsa.edu, Geology, University of Texas, San Antonio, TX 78249,

The Western Gneiss Region of Norway includes ~40,000 km2 of high-pressure rocks overlying ~10,000 km2 of ultrahigh-pressure rocks. The Caledonian HP-UHP metamorphism spanned 420- 400 Ma and reached 800° C at ~125 km depth. Exhumation was near-isothermal up to depths as shallow as 15–20 km. HP deformation diminishes toward the foreland: chaotic folds in the core of the orogen give way within ~20 km distance to moderately strong, but well-organized Caledonian fabrics, and within 100 km to only weakly overprinted Precambrian fabrics complete with Precambrian sphene and garnet; the stretching direction rotated from an early SE trend (e.g., the Stadlandet area) to a late NE trend (e.g., the Møre-Trøndelag Fault Zone and Nordfjord Mylonitic Shear Zone). At ~50 km depth, high-pressure minerals in the bulk gneiss reverted to a symplectite formed of low-pressure phases. Subsequent deformation was concentrated into specific zones: top-E motion along the eastern edge of the WGR and top- W extension along the western edge of the WGR (including the Nordfjord-Sogn Detachment Zone).

http://www.geol.ucsb.edu/faculty/hacker/#Norway

T32C-03

Foundering and Exhumation of UHP Terranes: Race Car or School Bus?

* Kylander-Clark, A R kylander@geol.ucsb.edu, UC Santa Barbara, Department of Earth Science, Santa Barbara, CA 93106-9630, United States
Hacker, B R hacker@geol.ucsb.edu, UC Santa Barbara, Department of Earth Science, Santa Barbara, CA 93106-9630, United States

Recent geochronologic data from the giant ultrahigh-pressure (UHP) terrane, in the Western Gneiss Region of Norway, indicate that subduction and exhumation were relatively slow (a few mm/yr), and that the terrane was exhumed to the surface as a relatively thick, coherent body. These conclusions are in stark contrast to those reached in previous studies of some of the best-studied, smaller UHP terranes and suggest that the processes that form and/or exhume small UHP terranes are fundamentally different from the processes that affect large UHP terranes. These differences may be the result of variations in the buoyancy forces of different proportions of subducted felsic crust, mafic crust, and mantle lithosphere. Initial collision occurs via the subduction of smaller portions of continental material, such as microcontinents or ribbon continents. Because the proportion of continental crust is small, the processes involved in early UHP terrane formation are dominated by the oceanic slab; subduction rates are fast because average plate densities are high, and, as a result, subduction angles are steep. Because these smaller, thinner portions of crust are weak, they deform easily and mix readily with the mantle. As the collision matures, thicker and larger portions of continental material—such as a continental margin—are subducted, and the subduction regime changes from one that was ocean dominated to one that is continent dominated. The increased buoyancy of the larger volume of continental crust resists the pull of the leading oceanic lithosphere; subduction shallows and plate rates slow. Because the downgoing continent is thick, it is strong, remains cohesive and has limited interaction with the mantle. Although the subduction regime during early orogenesis is distinct from that during late orogenesis, the degree of mountain building and crustal thickening may be similar in both stages as small volumes and fast flow rates of buoyant material give way to large volumes and slow flow rates.

T32C-04

Extension and Doming in (Ultra-)High-Pressure Terranes: Relationship to Syn-Convergent Exhumation of (U)HP Nappes

Jamieson, R A beckyj@dal.ca, Department of Earth Sciences, Dalhousie University, Halifax, NS B3H 4J1, Canada
* Warren, C J c.warren@open.ac.uk, Department of Earth and Environmental Sciences, The Open University, Milton Keynes, MK7 6AA, United Kingdom
Beaumont, C chris.beaumont@dal.ca, Department of Oceanography, Dalhousie University, Halifax, NS B3H 4J1, Canada
Butler, J P butlerjp@dal.ca, Department of Earth Sciences, Dalhousie University, Halifax, NS B3H 4J1, Canada

Many ultra-high-pressure (UHP) terranes are characterised by structural domes cored by nappe stacks comprising UHP eclogites in tectonic contact with overlying high-pressure (HP) and lower-grade rocks. Contacts between UHP and HP nappes are generally interpreted as thrusts, whereas contacts with overlying lower-grade rocks are typically normal-sense shear zones. Medium- and high-resolution (nested) numerical models for subduction and exhumation of continental crust in a subduction channel during the onset of collision provide an internally consistent explanation for these observations, including syn-convergent extension. The models involve subduction of a weak continental margin and stronger continental interior, and include strain weakening and reversible density changes accompanying metamorphic phase transformations. Results are interpreted in terms of the exhumation number, E, which expresses the relative contributions of Couette (down-channel) and Poiseuille (up-channel) flow components. During subduction, margin material progressively weakens, leading to diachronous detachment and exhumation of UHP rocks. Decoupling initiates at depth along a shear zone that propagates upwards. The buoyant UHP plume tunnels up the shear zone until it encounters HP material in the upper part of the subduction channel; the HP nappe is then folded over and exhumed by the rising UHP plume. The resulting structural dome is cored by the (U)HP nappe stack, with attenuated remanants of the suture zone overlying the UHP plume and its HP carapace. During the later stages of exhumation, a prominent low-angle extensional shear zone forms above the rising nappe stack, creating foreland-directed normal faults that separate the (U)HP nappes from lower- grade cover. Other nappe geometries can be produced by models significantly stronger or weaker than the reference model, but all include doming and accompanying extension that are driven by the buoyant rise of a substantial volume of UHP material. Model geometries and PTt paths are consistent with observations from Tso Morari and other natural examples.

T32C-05

Were the world's youngest eclogites (NW D'Entrecasteaux Islands, Papua New Guinea) exhumed in rising gneiss domes or by shear on a deep-seated fault?

* Little, T A tim.little@vuw.ac.nz, School of Geography, Environment & Earth Sciences, Victoria University, Wellington, 6140, New Zealand
Hacker, B hacker@geol.ucsb.edu, Institute of Crustal Studies, University of California, Santa Barbara, CA 93106-9630, United States
Seward, G seward@geol.ucsb.edu, Institute of Crustal Studies, University of California, Santa Barbara, CA 93106-9630, United States

The up to ~2.5 km-high gneiss domes of the NW D'Entrecasteaux Islands of Papua New Guinea host the world's youngest terrane of HP (eclogite-facies, ~2-4 Ma) to UHP (coesite-bearing) gneissic rocks (~8 Ma). Previous models for their exhumation at >2 cm/yr have called upon: 1) buoyant rise of crustal diapers, or 2) normal-slip on deeply penetrating faults. A recent variant of the latter suggests that a paleo- subduction zone near the southern edge of the Solomon Sea has been inverted as a result of microplate tectonics. We present structural, microstructural, and electron back-scatter diffraction data of lattice preferred orientations (LPO's) from gneisses of Goodenough and Fergusson Islands to further explore mechanisms of exhumation. Relict eclogite-facies assemblages occur in mafic dikes and boudins, but most HP deformational fabrics are overprinted. The enclosing felsic gneisses are pervaded by amphibolite-facies ductile fabrics formed during their exhumation from the lower crust. These migmatitic rocks (metatexites) were partially molten during their deformation at temperatures of 570-730°C and pressures of 7-11 kb, but today are dominated by solid-state fabrics. The gneisses are capped by remnants of an ultramafic sheet that did not experience HP metamorphism. Below the ultramafics is a ~1 km-thick carapace zone. These high-strain gneisses generally have domal fabrics parallel to, and gradational to, those in the underlying core zone, which they locally rework. Active NE-dipping normal faults on the NE flank of the domes cut across the ultramafic contact and are underlain by a m-thick zone of pseudotachylite-bearing S/C fabrics. A sweeping pattern of stretching lineations reveals a 3-D pattern of ductile flow. In both the carapace and upper core zone, lineations are mostly EW: subparallel to the long dimension of the domes and perpendicular to plate motion in the Woodlark Rift. At greater structural depth, within the core zone, they deflect to become more nearly plate-motion parallel. Shear indicators diverge across the dome crests, suggesting of an inward flow of deeper rocks into the dome; or are locally variable, consistent with bulk irrotational deformation. In the gneisses (both core and carapace), conjugate shear-band microstructures and near-orthorhombic quartz LPOs, and back-rotation of mantled porphyroclasts indicate that ductile strain in domes was near plane, but that it was not simple shear (and included significant vertical shortening). The LPO's of the deepest rocks record activity of the high-T prism-[c] and prism- slip systems, whereas the outermost carapace rocks record basal- and rhomb- slip. The data reveal that deformational temperatures increased toward the dome centers, rather than outwardly into the carapace. Quartz LPO's in both dome and carapace are of uniformly modest intensity (~2-3 times random). Feldspar LPO's suggest slip on the (010)[001] or (010)[100] systems, and in some cases a shear sense opposite to quartz. While we cannot resolve how the eclogitic rocks ascended isothermally from the mantle into the lower crust, the simplest model invokes diapiric ascent (with decompression melting), ponding and lateral spreading along the Moho during early Woodlark Basin rifting. Subsequent exhumation of these rocks from the lower crust involved continued upward movement and vertical shortening of the gneisses combined with subhorizontal rift-parallel flow. Finally, normal faulting and minor erosion exhumed these rocks through the ultramafic cover to their present levels.

T32C-06

Timing and Mechanisms of Oceanic Blueschist and Eclogite Exhumation : Implications for Subduction Mechanics

* Agard, P philippe.agard@upmc.fr, Lab. Tectonique, UMR CNRS 7072, Univ. P.M. Curie - Paris 6, T46-0, 2E, case 129 4 pl. Jussieu, PARIS, 75252, France
Yamato, P philippe.yamato@gmail.com, Lab. Tectonique, UMR CNRS 7072, Univ. P.M. Curie - Paris 6, T46-0, 2E, case 129 4 pl. Jussieu, PARIS, 75252, France
Monié, P patrick.monie@gm.univ-montp2.fr, Géosciences Montpellier, UMR CNRS 5243, Pl. E. Bataillon, Montpellier, 34000, France
Jolivet, L laurent. jolivet@upmc.fr, Lab. Tectonique, UMR CNRS 7072, Univ. P.M. Curie - Paris 6, T46-0, 2E, case 129 4 pl. Jussieu, PARIS, 75252, France
Burov, E burov@lgs.jussieu.fr, Lab. Tectonique, UMR CNRS 7072, Univ. P.M. Curie - Paris 6, T46-0, 2E, case 129 4 pl. Jussieu, PARIS, 75252, France

Understanding what controls the detachment and migration of oceanic crustal slices along the subduction channel is crucial to constrain subduction mechanics. For this reason, we compiled key information pertaining to the burial and exhumation of oceanic blueschists and eclogites worldwide (shape of exhumation P-T-t paths, exhumation velocities, timing of exhumation with respect to the convergence process, convergence velocities, volume of exhumed rocks). In contrast with the fast (> cm/yr), buoyancy-driven exhumation of continental rocks, oceanic exhumation velocities for high-pressure low-temperature oceanic rocks, whether sedimentary or crustal, are usually on the order of the mm/yr. The sediments are characterized by the continuity of the P-T conditions and the importance of accretionary processes, whereas blueschist and eclogite mafic bodies are systematically associated with serpentinites and/or a mechanically weak matrix and crop out in an internal position in the orogen. Oceanic crust rarely records P conditions > 2.0-2.3 GPa, which suggests the existence of maximum depths for the sampling of slab-derived oceanic crust. Natural observations and calculations of the net buoyancy of the oceanic crust suggest that beyond depths around 70 km there are either not enough serpentinites and/or they are not light enough to compensate the negative buoyancy of the crust. This survey demonstrates that short-lived (< 15 My), discontinuous exhumation is the rule for the oceanic crust. Exhumation takes place either early (group 1: Franciscan, Chile), late (group 2: New Caledonia, W. Alps) or incidentally (group 3: SE Zagros, Himalayas, Andes, N. Cuba) during the subduction history. This discontinuous exhumation is likely permitted by the specific thermal regime following the onset of a young, warm subduction (group 1), by continental subduction (group 2) or by a major, geodynamic modification of convergence across the subduction zone (group 3). In addition, we stress that any model of plate-slab coupling should account for the evidence of short-lived, coeval exhumation occurring along thousands of km (from Turkey to the Himalayas in the case of the Neotethyan subduction).

T32C-07

The contribution of geochronology to determination of burial and exhumation rates of (U)HP rocks

* Parrish, R R rrp@nigl.nerc.ac.uk, Dept Geology University of Leicester & NERC Isotope Geoscience Laboratory, British Geological Survey, Keyworth Notts, NG12 5GG, United Kingdom
Cottle, J jott@bgs.ac.uk, NERC Isotope Geoscience Laboratory, British Geological Survey, Keyworth Notts, NG12 5GG, United Kingdom
Condon, D dcondon@bgs.ac.uk, NERC Isotope Geoscience Laboratory, British Geological Survey, Keyworth Notts, NG12 5GG, United Kingdom

The seemingly extraordinary rapid and deep subduction of buoyant continental crust and its return to the surface is proving rather more the rule than the exception in continental collision zones, notwithstanding the patchy preservation of such rocks. Modelling and buoyancy contrasts suggest that following rapid subduction and ductile de-coupling from the downgoing slab, the rate of exhumation is first very rapid within the mantle but slower as the buoyancy contrast is reduced in the crust. One test of models is the quantitative determination of the P-t path of real samples. Geochronology is pivotal in this regard and with rapid exhumation (¡Ý1 cm/a), it is paramount to produce precise and robust mineral growth and cooling ages of a variety of pressure- and temperature-sensitive minerals, ideally in their petrographic context, using a variety of chronometers, so that the geochronology can resolve the rapid rates. Issues of high relevance to this application of geochronology are (1) resolving and applying the ~0.5-1.0% decay constant bias between (40K)40Ar-39Ar dates and U-Pb dates, especially critical for older orogen exhumation rates (i.e. Caledonides); (2) correctly interpreting U-Pb ages when complex U-Pb systematics are likely to be present; (3) using prograde mineral chronology during cool subduction with minerals of high closure temperature (allanite-epidote, garnet, monazite, zircon, ¡À titanite); (3) determining P-T conditions of growth of these minerals using metamorphic modelling and chemical mapping; dating minerals in their petrographic context wherever possible; (5) making the most of minerals like zircon through innovative dating and inclusion petrology in very thin overgrowths; (5) and assessing growth v. closure temperature interpretation of dated minerals using experimental and empirical diffusion data. These points will be illustrated by examples of studies from Kaghan Himalayan, Caledonide and Chinese UHP rocks to suggest fruitful multi-technique approaches as a way forward.

T32C-08 INVITED

Interaction of metamorphism, fluids and deformation in exhuming subducted continental crust, field evidence and a model

* JOLIVET, L laurent.jolivet@upmc.fr, UPMC-Paris6, Laboratoire de Tectonique, UMR 7072, 4 Place Jussieu, Paris, 75252, France
Labrousse, L , UPMC-Paris6, Laboratoire de Tectonique, UMR 7072, 4 Place Jussieu, Paris, 75252, France
Hetényi, G , Ecole Normale Supérieure, Laboratoire de Géologie, UMR 8538, 24 Rue Lhomond, Paris, 75231, France
Huet, B , UPMC-Paris6, Laboratoire de Tectonique, UMR 7072, 4 Place Jussieu, Paris, 75252, France
Raimbourg, H , UPMC-Paris6, Laboratoire de Tectonique, UMR 7072, 4 Place Jussieu, Paris, 75252, France
Cattin, R , Ecole Normale Supérieure, Laboratoire de Géologie, UMR 8538, 24 Rue Lhomond, Paris, 75231, France

Exhuming pieces of continental crust from the depths of a subduction channel involves a competition between buoyancy and viscosity, so that lighter and less viscous units will exhume more efficiently. In terms of geological evolution, two conditions are required: (1) once they have been dragged down to large depth, tectonic units must be decoupled from the subducting lithosphere and, (2) they must be allowed to move upward within the subduction channel. Both processes involve considerable deformation along the units margins and this deformation is aided by fluids and metamorphism. It is a frequent observation that deformation is totally absent or very weak along the prograde path and this is not only because it has been erased by later events. The examples of the Norwegian Caledonides or the Aegean, or even the Alps, show that the first significant deformation event is recorded near the peak of pressure, thus at maximum depth. This is in line with the idea that the more resistant a rock unit is, the deeper is can be dragged along with the subducting plate, and UHP metamorphics are indeed basement rocks in most cases. The first deformation is sometimes partly brittle as suggested by the Bergen Arcs example. Fluids then invade fractures or shear zones and initiate metamorphic recrystallisation at peak pressure. This further induces a local density increase associated with a drop in strength and strain localisation ensues, that in turns promotes recristallisation. Large and weak shear zones progressively form and the tectonic unit is then decoupled from the subducting lithosphere. Afterward, the piece of continental crust makes its way upward in the subduction channel, limited by a thrust along its base and a normal "extensional" shear zone at its top. Then again, the interaction between fluid and deformation is important during retrogression into the blueschists (Aegean, Alps) or the amphibolite facies (Caledonides). Large scale ductile shear zones accommodate the exhumation during progressively less and less severe metamorphic conditions. In the vicinity of the brittle-ductile transition zone fluids from the surface invade the shear zones and further facilitate strain localisation. We discuss a simple kinematic model that integrates this sequence of events in various geodynamic contexts.