consequences of continental subduction on forearc basin...

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Tectonophysics 466 (2

Consequences of continental subduction on forearc basin and accretionarywedge deformation in SE Taiwan: Insights from analogue modeling

Jacques Malavieille ⁎, Ghislain Trullenque 1

Laboratoire Dynamique de la Lithosphère, UMR 5573, University Montpellier 2, place E. Bataillon, 34095 Montpellier Cedex 5, France

Available online 22 November 2007

Abstract

In southeastern Taiwan a slice of forearc basement belonging to the Philippine Sea Plate upper-plate is suspected to subduct under the Luzon arc asa consequence of the transition from oceanic to incipient continental subduction. Effects on the morphology, deformation, geometry of structures andtectonic evolution of the orogenic wedge in the collision area are numerous. This study examines the impact of forearc lithosphere subduction onforearc basin and accretionary wedge deformation. A morpho-structural analysis of the geological features observed onland and offshore allowsdescribing in detail the complex deformation suffered by the area. A combined approach by analogue modeling is applied to better understand thephenomenon. Comparison between nature and experimental results shows that subduction of a forearc basement slice induces intense shortening andconcomitant deformation in the forearc domain. Such process involves deformation of the forearc basin previously developed in a setting of oceanicsubduction. Sediments of the forearc basin are involved in the growth of a new thrust ridge backthrusted against the basement slope of the volcanic arcedifice. Sediments coming from the growing orogenic wedge are trapped in the trough developed between its backpart and the topographic high of thenew rising ridge. A syn-collisional orogenic basin develops which structural evolution characterizes the progressive shortening of the forearc domain.Most of the deformation and tectonic events recorded offshore or onland in the complex area south of Taiwan can be explained using results of ourspecific modeling which well describe the tectonic processes associated with continental subduction under a volcanic arc.© 2007 Elsevier B.V. All rights reserved.

Keywords: Taiwan; Continental subduction; Forearc deformation; Syn-collisional orogenic basin; Analogue modeling

1. Introduction

In convergent settings, the transition between oceanic andcontinental subduction induces major changes in the mechanicalboundary conditions at plates boundary. Simple geologicalcomparison from south to north of Taiwan shows that a largepiece of the oceanic accretionary system is missing in the domaininvolving continental subduction, where remnants of the volcanicarc edifice (coastal range) are directly juxtaposed with meta-morphic continental rocks of the central range. Such setting isdifficult to reconcile with classical arc-continent collision models.Recent works, some based on physical and numerical modeling atlithospheric scale (Chemenda et al., 1997; Tang and Chemenda,2000; Chemenda et al., 2001; Boutelier and Chemenda, 2003),

⁎ Corresponding author.E-mail address: [email protected] (J. Malavieille).

1 Presently at: Faculty of Earth Sciences, Utrecht University, P.O. Box 80.021,3508 TA Utrecht, The Netherlands.

0040-1951/$ - see front matter © 2007 Elsevier B.V. All rights reserved.doi:10.1016/j.tecto.2007.11.016

others based on geological and geophysical observations onlandand offshore Taiwan (e.g., Malavieille et al., 1999, 2002; McIntoshet al., 2005), have demonstrated that an important tectonic processoccurswhich is characterized by subduction of a forearc lithosphereslice under the oceanic lithosphere constituting the upper-plate. Atthe beginning of the process, the subduction of the continentalmargin strongly increases the stress and strain in the upper-plate(Shemenda, 1994; Lallemand, 1999; Tang and Chemenda, 2000),sometimes involving failure and then subduction of a lithospheresliver from the forearc domain. The effects of these deep processeson morphology, internal structure and tectonic evolution of theaccretionarywedge-forearc basin system are numerous but scarcelystudied until now. Using sandbox models, we have studied theimpact of this geodynamic process on deformation at the scale ofthe accretionary wedge. We model a setting in which a continentalmargin is subducting under an oceanic lithosphere bearing amaturevolcanic arc, inducing subduction of forearc lithosphere. Theresults of the modeling are compared with geological observationsfrom southeast Taiwan and a new interpretation is proposed for the

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http://dx.doi.org/10.1016/j.tecto.2007.11.016

378 J. Malavieille, G. Trullenque / Tectonophysics 466 (2009) 377–394

morphostructural evolution of the presently active transition fromoceanic to continental subduction occurring in this area.

2. General setting of Taiwan

Arc-Continent collision is classically considered to be exem-plified by the subduction of the continental margin of China underthe Luzon island arc (e.g, Sibuet, J.-C., and Hsu, S.-K., 1997).

Fig. 1. Morphostructural map of the Taiwan area showing the main tectonic units whicFig. 11 are localized (blue lines). CP, Coastal Plain; WF, Western Foothills; HSR, HsCR, Coastal Range; SLT, “Southern Longitudinal Trough” orogenic basin; HP, HengcTT, Taitung Trough; MAW, Manila Accretionary Wedge; FB, Forearc Basin; OCT,

Two plates are involved in the complex tectonic setting thatsurrounds the Taiwan orogen, the Philippine Sea Plate (PSP),and the Eurasian plate (Fig. 1). Northeast of the Taiwan area, thePSP is being subducted beneath the Ryukyu arc, which belongsto the Chinese continental margin. South of the Taiwan Island,the oceanic lithosphere of the South China Sea subducts beneaththe PSP, inducing the volcanism of the Luzon arc. The relativemotion between the PSP and the Eurasian plate has resulted in

h characterizes the transition from oceanic to continental subduction. Sections ofueshan Range; LF, Lishan Fault; TC, Tananao Complex; BR, Backbone Range;hun Peninsula; HR, Hengchun Ridge; HtR, Huatung Ridge; KS, Kaoping Slope;inferred Ocean Continent Transition.

379J. Malavieille, G. Trullenque / Tectonophysics 466 (2009) 377–394

the progressive subduction of the Chinese continental marginand the development of the Taiwan mountain belt.

Global kinematics indicate that the PSP is currently movingnorthwestward (N306°±1° azimuth), with respect to the Eurasianplate (Seno, 1977; Seno et al., 1993) at a rate ranging between 80–83mm/yr (GPS data, Yu et al., 1997; Lallemand and Liu, 1998) or90 mm/yr (REVEL model, Sella et al., 2002). Because the Asiancontinental margin trends diagonally with the Luzon arc, the arc-continent collision is oblique and the point of continental sub-duction rapidly migrates southward (Suppe, 1984). The oceaniclithosphere of the South China Sea was subsequently subductedbeneath the PSP along theManila Trench in the earlyMiocene, assuggested by the Neogene age of associated volcanism along theLuzon Arc (Ho, 1986; Richard et al., 1986). The Manila accre-tionary wedge has developed between the two plates (Fig. 1) andis still growing today south of 21°20′N (Lewis and Hayes, 1983;Hayes and Lewis, 1984; Lewis and Hayes, 1984, 1989). North of21°20′ N, the wedge becomes incorporated in the domain ofcontinental margin subduction, involving progressively lower tomiddle Miocene slope and trench sediments (Reed et al., 1992).The southern tip of Taiwan Island represents the uplifted internaldomain of the oceanic accretionary wedge currently undergoingthe effects of the collision (Lundberg and Dorsey, 1990; Reedet al., 1992; Huang et al., 1997). The backpart domain of thewedge extends offshore southward of the Hengchun Peninsula inthe form of the Hengchun Ridge as far as 20°30′ N (Fig. 1). Arealistic scenario for the tectonic evolution of the submarineaccretionary wedge has been proposed by Huang et al. (1997). Intheir model, the NW–SE oriented Kaoping Slope west of thesubduction wedge of the Hengchun Ridge represents the part ofthe prism associated with the incipient subduction of the chinesecontinental margin (e.g. Huang et al., 1997; Liu et al., 1997). Thetransition between oceanic and continental crust (OCT, see Fig. 1)

Fig. 2. Sketch of the “sandbox” deformation apparatus. S1, Velocity discontinuityassociated to the retreat of the mobile plate.

in the Eurasian plate is marked approximately by the 2500 misobath (Letouzey et al., 1988). Although being oriented ap-proximately N 70° E to the southwest of Taiwan, the present trendof this boundary is not regular suggesting that the southwardpropagation of collision is not a stable and continuous process asoften supposed.

The geologic setting of the Taiwan orogenic wedge itself canbe summarized as follows. The sedimentary cover of the Chinesecontinental margin (see Taiwan Strait in Fig. 1) was accreted inthe northwestern part of the island, and it is still accreting in thesouthwestern part, against a backstop formed by the pre-Tertiaryrocks of the Central Range (e.g. Lu and Malavieille, 1994).Shallow marine sequences of the passive continental margin andforeland sequences constitute the deformed units of the CoastalPlain,Western foothills and Hsüehshan Range (Ho, 1982, 1988).During convergence, they were progressively accreted to themountain belt along a series of east-dipping thrusts. The CentralRange includes the Eocene and Miocene (but not Oligocene)metamorphic Backbone Range. The Lishan Fault, west of thesubduction wedge, is a high-angle west dipping fault (Lee et al.,1997), which separates the western Backbone Range from theEocene–Oligocene units of the Hsüehshan Range, both of themforming the Slate belt (Ho, 1986; Angelier et al., 1990; Tenget al., 1991; Clark et al., 1993; Tillman and Byrne, 1995). TheWestern Foothills correspond to a fold-and-thrust belt affectingOligo–Miocene strata overlain by a 4-km-thick sequence ofPliocene–Quaternary molasse (Lu and Hsü, 1992). This fore-land thrust belt seems inactive north of 24° N, but it is stillgrowing south of this latitude as shown by seismicity and GPSmeasurements (Yu et al., 1997). The Central Range is bounded tothe east by the Longitudinal Valley, which separates the CentralRange from the Coastal Range (i.e., northernmost segment of theLuzon volcanic arc). Deformation of the PSP lithosphere within

associated to the displacement of the Mylar sheet; S2, Velocity discontinuity


the Coastal Range is suggested by the 50-km-thick seismogeniczone beneath the arc domain (Wu et al., 1997). A large part ofthe Coastal Range is still well coupled to the PSP, as attestedto by the GPS velocities of 63±9 mm/yr in the direction ofN314°±8°, except north of 23°40′ N where rates dramaticallydrop to 8–43 mm/yr along the azimuths N292°–352° (Yu et al.,1997). About 80–90 mm/yr of plate convergence is taken up inthe offshore area north of 24° N, whereas south of 24° N, theconvergence is distributed across the island,with about 30–40mm/yr accommodated in the western foothills (Simoës, 2005), 30 mm/yr in the Longitudinal Valley area (Angelier et al., 1997), andonland and offshore across the other thrusts of the Coastal Rangeunits shown in Fig. 1 (Yu et al., 1997; Deffontaines et al., 2001;Malavieille et al., 2002; Shyu et al., 2005).

The Luzon island arc and the associated Manila Trench aregenerally considered as early Miocene in age (Juang and Bellon1984). The northernmost present-day activity of the arc isobserved at the latitudes of the Batan Islands. Younger ages, asrecent as 30 ka, were also found using K–Ar dating on Lutaoand Hsiaolanyu (a small island located south of Lanyu) islands.The activity of the northern segment thus probably ceased during

Fig. 3. Five evolutionary steps of experiment 3. Friction was low at the base of the sarrows outline the domain affected by active shortening at each stage.

the Quaternary at the latitude of the islands of Lutao and Lanyu(Yang et al., 1996). A progressive increase in continental con-tamination of andesitic magmas correlates with progressivelyyounger ages in Coastal Range volcanic rocks. This progressionreflects the systematic increase through time of continentallyderived sediment entering the Manila Trench (Dorsey, 1992), andthe transition from oceanic to continental subduction inducingsubduction of a slice of forearc lithosphere (e.g. Malavieille et al.,2002), shortly before the cessation of island-arc magmatism.North–south changes in the geology and morphology of theTaiwan orogenic wedge reflect the increasing imprint of theChinese margin “continental subduction”.

3. Analogue modeling

At a crustal scale, the structure and dynamics of accretionarywedges has been widely studied using analogue modelingtechniques, allowing a better knowledge of the various processescontrolling their growth. Some of them focused on deformation,structure geometry and kinematics (Malavieille, 1984; Mulugeta,1988; Calassou et al., 1993; Lu and Malavieille, 1994; Merle and

and cake, both on the mylar sheet and on the “forearc” plastic plate. The empty


Abidi, 1995; Gutscher et al., 1996;Mugnier et al., 1997; Gutscheret al., 1998a,b; Dominguez et al., 1998a,b, 2000; Gutscher et al.,2001; Casas et al., 2001; Cobbold et al., 2001; Kukowski et al.,2002; Martinez et al., 2002; Marques and Cobbold, 2002; Smitet al., 2003), others analyzed the impact of surface processes suchas syntectonic sedimentation (Malavieille et al., 1993; Larroqueet al., 1995; Storti and Mc Clay, 1995; Leturmy et al., 2000;Barrier et al., 2002; Del Castello et al., 2004) or syntectonicerosion on the dynamics of the orogenic wedge (Persson andSokoutis, 2002; Persson et al., 2004; Konstantinovskaia andMalavieille, 2005; Hoth et al., 2006). At lithospheric scale,subduction processes have been studied using scaled modelsdesigned to be analogues for lithosphere deformation (Chemendaet al., 1995, 1997). In this frame, specific experiments devoted tostudy the effects of continental subduction on upper-plate islandarcs, have shown that the subduction of slices of fore-arclithosphere can occur under specific mechanical boundaryconditions (e.g. Chemenda et al., 2001; Boutelier and Chemenda,2003). They show that subduction of a continentalmargin beneatha volcanic arc, may induce failure of the arc lithosphere at thevicinity of the volcanic arc, subsequent shortening involving

Fig. 4. Experiment 7. Friction was low on the mylar sheet at the base

slicing and subduction of part of the fore-arc domain. In such ageodynamic setting, processes and deformations occurring in theupper levels of the crust (i.e., at the scale of the accretionarywedge or the forearc basin) are poorly known.Our study concernsthe modeling of the accretionary wedge–forearc basin deforma-tion and evolution, in relation with the subduction of a slice ofupper-plate lithosphere in front of a volcanic arc. The aim was tobetter understand the evolution of the complex deformation thatoccurs southeast of Taiwan due to the progressive implication ofthe Chinese continental margin in the subduction. The geologicalfeatures suspected to be correlatedwith such a tectonic process areanalyzed in the light of our modeling results.

Experimental apparatus and procedure: Each experiment wasperformed under normal gravity using an apparatus (Fig. 2)which simulates the basic geometry and general kinematics of asubduction zone. The classical sandbox device, close to the oneused by Malavieille (1984) and Lallemand et al. (1992), isconstituted by a horizontal basement bounded by two sidewallglasses. A 10 cm wide mylar sheet (analogue of the oceanicplate), lying on the horizontal plate, is pulled beneath a rigidbackstop allowing more than 1.5 m of convergence for each

of the sand cake, and high on top of the “forearc” plastic plate.


experiment. Different roughness of the plastic sheet are used totest the effect of different frictions at the base of the sand cake.The rigid backstop (fixed) presents a shape with a low dippingslope (15°) that represents the volcanic edifice of the island arcagainst which the sediments are deformed. To model thespecific kinematic boundary conditions imposed by thesubduction of a forearc basement slice in front of the volcanicarc, we add a thin mobile plate (PVC plastic) on the mylar sheetin front of the rigid backstop. The buttress that bounds thesandbox remains fixed during the experiment, whereas theplastic plate can slide beneath it, involving progressive short-ening of the forearc domain during convergence. The frictioncan be adapted on the backstop surface and on the top surface ofthe mobile plate.

On the mylar sheet, 3 cm of successive coloured sand layerssimulate the oceanic sediments (Fig. 2). They allow building ofthe initial accretionary wedge (Manila accretionary wedge) thatdeveloped before the beginning of continental subduction. Thesame material is used to progressively fill the trough (forearc

Fig. 5. Experiment 5. Friction was high on the mylar sheet at the ba

basin) that develops between the rear of the model sand wedge(accretionary prism) and the rigid backstop (front of thevolcanic arc). The back motion of the PVC plate (analogue ofthe forearc basement) is controlled during the experiment run.

The aeolian sand used in this study is rounded with a grainsize of less than 300 micrometers and a density of 1690 kg/m3.The internal coefficient of friction is 0.57 and the cohesionCo=20 Pa. The model materials have frictional propertiessatisfying the Coulomb theory (Dahlen et al., 1984; Dahlen,1984) and thus, it is a fair analogue of the rocks of the upper crust(Krantz, 1991). Sandbox scaling has been widely discussed (seefor example; Lallemand et al., 1992, 1994; Kukowski et al.,1994; Gutscher et al., 1996, 1998b; Kukowski et al., 2002;Lohrman et al., 2003) and 1 cm in our experiment is roughlyequivalent to 1 km in nature. The same dry sand is used tosimulate the sediments of the accretionary wedge and thesediments filling the basin (analogue of the forearc basin)located between the back of the thrust wedge and the rigidbackstop. Two cameras and one video recorder recorded each

se of the sand cake, and low on top the “forearc” plastic plate.


stage of deformation. Structural interpretations are based onplanar views recorded at the same time as the morphologicalperspective views presented.

Each experiment has been performed following three stages.

1) During the first stage, the PVC plate (forearc basement)remains fixed to the rigid backstop. Motion of the mylar sheetallows the growth of a typical doubly vergent sand wedgewhich geometry is controlled by the velocity break (S1)located at the tip of the PVC plate. The internal deformationof the wedge is characterized by dominant frontward-vergentthrusts with regular narrow spacing and frontward sequencesof thrust development on one side and, localized back-thrusting on the backside. Backthrusting controls basindevelopment during shortening and syntectonic sedimenta-tion (see a detailed study of this process in Malavieille et al.,1993; Larroque et al., 1995).

Fig. 6. Experiment 6. Friction was high on the mylar sheet at the ba

2) During the second stage, a mechanical coupling is realizedbetween the mylar sheet and the PVC plate. Then, a secondvelocity discontinuity (S2) works at the tip of the rigidbackstop inducing shortening in the “forearc“ domain. Such acoupling can be total (this is the case in four of the fiveexperiments presented) or partitioned (this has been tested onexperiment 4). In the first situation, the retreat of the PVC plateoccurs at the same velocity as the motion of the mylar sheetmaking the S1 velocity break inactive whereas S2 concentratesthe deformation. The experiment 4 was designed to test a morecomplex tectonic situation in which the rate of subduction ofthe forearc slice is supposed to be slower than the mainsubduction. It has been run to check the effect of a differentialvelocity between S1 and S2, the two velocity discontinuitiesworking together during shortening. The equivalent of a syn-orogenic basin is initiated since the beginning of this stage. Inthe experiments syn-deformation deposit of sand layers with

se of the sand cake, and high on top the “forearc” plastic plate.


different colours allows to visualize the shape and deformationstate of the new “piggy-back“ orogenic basin.

3) Third stage: after complete removal of the PVC plateshortening goes on some tens of centimeters until the endof the experiment.

In the next part, we describe and compare the results obtainedon several laboratory experiments varying two main parameters,the friction at the base of the sediments and the relative shorteningratio between the rigid backstop, the moving PVC plate and basalplastic sheet. The low and high basal friction in the different partsof the models are obtained respectively by polishing (low friction)the rigid backstop, the PVC plate and the basal plastic sheet and bysticking sand grains on their surfaces (high friction). These majorchanges in boundary conditions induce the specific deformationand evolution suffered by the prism and the associated basinsdeveloped on its backpart.

Fig. 7. Experiment 4. Friction was low on the mylar sheet at the base of the sand cake,of the mylar sheet (V mylar on the Fig. 7), is higher than the velocity of the PVC plate

4. Results of experiments

A series of five significant experiments have been analyzedallowing to determine the main effects of the different testedparameters. One of them (experiment 3) is described in detail(Fig. 3), whereas, as the differences in the others concern minorpoints of models evolution, only their original characters aresummarized.

In experiment 3, basal friction on the plastic sheet was lowand friction on top of the PCV plate and rigid backstop was lowtoo. Kinematics of deformation is analyzed using photographstaken each 2.5 cm of shortening. During shortening, the step-by-step input of sand (sediments) in the back part of thedeveloping thrust wedge allows filling of a syntectonic basin (ina forearc setting). The sand input is generally chosen to partlyfill the topographic low that develops between the domain ofbackthrusting in the wedge (domain of major topographic high

and low on top the “forearc” plastic plate. The PVC plate is removed, the velocity(V PVC). The reference is given relative to the fixed backstop (V backstop=0).


in actual oceanic wedges) and the rigid backstop (equivalent ofthe inner slope of the volcanic edifice). This choice is based onobservation of the present area extent of the forearc basindeveloped south of Taiwan, where the accretionary wedge issimple. The wedge domains affected by faulting and deforma-tion are shown on figures by the blue arrows.

During the first stage of modeling (about 40 cm shortening,Fig. 3a and b), the PVC plate remains coupled with the rigidbackstop. A typical low-friction wedge develops which doublevergence is controlled by the velocity discontinuity located atthe tip of the PVC plate (S1 on all the figures). The wedgegrowths rapidly by frontal accretion of small thrust unitsbounded by a set of antithetic thrusts. The dip of the slope islow. The zone of backthrusting developed at the rear of thewedge allows the growth of the basin which deposits remainundeformed except at the vicinity of the major backthrust.

When the size of the model wedge and associated basin areassumed to be reasonably comparable to its natural equivalent (theoceanic accretionary wedge presently observed south of Taiwan,far from the collision zone, i.e. south of 21° N), we initiate theretreat of the PVC plate (by coupling the plate with the plasticsheet underneath) simulating forearc subduction. This inducesmajor changes in the wedge dynamics characterizing the secondtectonic stage. The frontal growth of the wedge stops and thedeformation concentrates now at the back part of the system, in

Fig. 8. All experiments drawn at last deformation stage, show

front of the rigid backstop. A major backthrust allows back-thrusting of the basin sequences onto the backstop. A series of lowdip thrusts initiate from the new velocity discontinuity (S2 on thefigures), they cut and deform the layers of the basin developing atopographic ridge against the backstop (Fig. 3, stage c). When thenew ridge reaches a critical slope, it growth forward and mostof the basin sequences are thrusted on the rear part of the ac-cretionary wedge.

As shortening increases, deformation allows a new syntectonicbasin to be developed in the synformal structure bounded bythe forearc ridge and the back of the accretionary wedge (Fig. 3,stage d). This new “orogenic basin“ is strongly deformed due tosyn-shortening sedimentation. During the last steps of the PVCplate retreat and after its complete removal, the main décollementlocated at the base of the thrust wedge is reactivated allowingwedge growth by frontal accretion of new tectonic units. Then,thrust partitionning resumes, S2 controls wedge growth and thewhole model behaves again as a classical accretionary wedge(Fig. 3, stage d).

The differences induced by parameter changes in each of theother experiments are listed below.

In the experiment 7, the friction on top of the PVC plate andrigid backstop is high. The general evolution of the sandwedge(Fig. 4, stages a, b, c) is quite similar to experiment 3, but thenew ridge developed against the buttress during retreat of the

ing the geometry and structure of the main tectonic units.


PVC plate overthrusts the back part of the accretionary wedge,giving an open syncline geometry to the deformed basin in thelast stages of shortening (Fig. 4, stages d, e). The orogenic basinis mainly affected by forward thrusting.

In the experiment 5, the friction is high on the mylar sheetwhereas it is low on top of the PVC plate and backstop. Themodel shows the characters of typical high friction wedge with ahigh dipping slope and forward growth by stacking of longthrust units (Fig. 5, stages a, b). Here again, as in exp. 7, retreatof the PVC plate induces ridge growth and overthrusting of thesyntectonic sequences of the basin on the rear part of theaccretionary wedge (Fig. 5, stages c, d). After complete removalof PVC plate, as deformation resumes, the whole thrust wedgegrowths again and a new out of sequence backthrust develops atthe boundary between the deformed basin and the rear of thewedge (Fig. 5, stage e). Backthrusting is more developed in thisexperiment and affects the orogenic basin too.

In the experiment 6, the basal friction is high everywhere.Result is very close to model 5 (Fig. 6, stages a, b). Retreat of thePVC plate induces growing of a doubly vergent ridge above S2

Table 1Table summarizing the main characters of the five experiments described in the tex

Experimentnumber

Exp.7 Exp.6 Ex

Friction on top ofthe movingsheet

Low High Hig

Friction on top ofthe mobile PVCplate

High High Lo

Friction on top ofthe fixedbackstop

High High Lo

Motion of velocitybreaks S1 andS2 relative tofixed upper-plate (tip offixed backstop)

Step1: V lower-plate=Cste andV moving plate=0Step 2: V lower-plateNV moving plateN0

Step1: V lower-plate=Cste and V movingplate=0Step 2: V lower-plateNV moving plateN0

SteCsplaSteNV

Structure of theaccretionarywedge

Basal décollement andfrontal accretion of smallthrust units bounded by aset of antithetic thrusts.Minor backthrusting inthe retro-wedge

Forward growth bystacking of long thrustunits. Major backthrustingin the retro-wedgecontrols basin formation.

Fostauniincon

Dip of the slope Low High HigMain stages ofdeformation inthe forearc basin

1 — arc-vergentmain thrust+minorforethrusts2 — majoroverthrusting of thebasins on the rear partof the wedge

1 — deformation againstthe backstop. Arc-vergentmain thrust+minor forethrusts2 — major backthrusting ofthe basin on the backstop.Antithetic forethrust cuts therear part of the wedge

1 —bacthr2 —fora c

Structure of theorogenic basin

Large synformalstructure controlledby antithetic thrusts(pop down)

Narrow asymmetric basinresting unconformably onthe rear slope of the wedge.Backstop side is deformedby small forethrusts.

Wiwitstruant

(Fig. 6, stages c, d). During last stages of shortening, the lastformed out of sequence forethrust cuts the back of the accretionarywedge,whereas thrusting resumes at the front (Fig. 6, stage e). Theorogenic basin is relatively little affected by faulting as it ispassively displaced on top of the sequences of the previous basin.

In the experiment 4, since the PVC plate is removed, thevelocity of the mylar sheet (V mylar on the Fig. 7), is higherthan the velocity of the PVC plate (V PVC). The reference isgiven relative to the fixed backstop (V backstop=0). It wasdesigned to test a more complex tectonic situation in which therate of subduction of the forearc slice is supposed to be slowerthan the main subduction. The basal friction was loweverywhere in the model as for experiment 3. The evolutionof the sandwedge is similar as exp. 3. As both velocity breaks S1and S2 act together, deformation of the thrust wedge goes onwhile the domain of the basin is deformed (Fig. 7, c, d, e).Backthrusting develops at the rear of the thrust wedge, whereasa new thrust ridge growth in the basin against the backstop.Both thrust systems work concomitantly until the end of PVCplate retreat. At the end of shortening, the deformed basin

t

p.5 Exp.3 Exp.4

h Low Low

w Low Low

w Low Low

p1: V lower-plate=te and V movingte=0p 2: V lower-platemoving plateN0

Step1: V lower-plate=Cste andV moving plate=0Step 2: V lower-plateNV moving plateN0

Step1: V lower-plate=Cste andV moving plate=0Step2: V lower-plate=0 and V movingplate=Cste. S1 & S2acting together

rward growth bycking of long thrustts. Major backthrustingthe retro-wedgetrols basin formation.

Basal décollementand frontal accretionof small thrustunits bounded by aset of antithetic thrusts.Major backthrustingin the retro-wedge

Basal décollement andfrontal accretion ofsmall thrust unitsbounded by a setof antithetic thrusts.Major backthrustingin the retro-wedge

h Low Lowdeformation against the

kstop. Arc-vergent mainust+minor forethrusts

basal décollement in theearc controls shortening inomplex synformal basin

1 — arc-vergent mainthrust+minor forethrusts2 — major shortening ofthe basins between therear part of the wedgeand the backstop

1 — arc-vergent mainthrust+minorforethrusts2 — major shorteningof the basins betweenthe rear part ofthe wedgeand the backstop

de and shallow basinh a complex synformalcture controlled byithetic thrusts (pop down)

Small synformal structurecontrolled by antitheticthrusts (pop down)

Small “pop down“structure on top ofdeformed forearcbasin


overthrusts the rear part of the accretionary wedge. It results in asynformal basin structure bounded by two antithetic thrusts andcarrying in its center a small “orogenic basin” (Fig. 7, stage e).The orogenic basin is mainly deformed by backthrusting.

The Fig. 8 and Table 1 summarize the main characters ofdeformation for the five experiments.

5. Insights of modeling results on the structural evolution ofsouthern Taiwan

The complex geology and tectonic features of the area south ofTaiwan are presented using original structural maps (Figs. 1

Fig. 9. Detailedmorphostructural sketchmap of southern Taiwan area. Onland and offs2— thrust (teeth on upper plate), 3— inactive thrust (teeth on upper plate), 4— foldrocks of the Coastal Range, 9—mud volcano, 10—mass wasting. A and B lines shoin Fig. 1.

and 9) and geologic cross sections (Fig. 10). The maps andsections have been designed combining published and unpub-lished terrestrial and marine data. They include personal fieldobservations in the southern part of the Taiwan belt, new analysisof seismic lines obtained on the area during the 1996 RVL'Atalante, ACT cruise (Lallemand and Liu, 1997) or older linesof the 1990 Moana Cruise (given by the courtesy of C-S Liu) aswell as insights of modeling results on the structural evolution ofsouthern Taiwan.

The transition from oceanic to continental subduction alongthe Manila Trench occurs near 22° N, but the impact ondeformation of this major change in the nature of the two plates

hore structures and tectonic units are correlated. Symbols and patterns: 1— fault,axis, 5—minor fault, 6— drainage, 7— recent collisional basin, 8— volcanicw location of detailed geological cross sections of Fig. 10. Same abbreviations as

Fig. 10. Detailed geologic cross-sections in the domain of incipient continental subduction.


is observed as far south as 21° N. Three main morphostructuraldomains characterize this transition:

1) Domain of oceanic subduction.

South of 21° N (Fig. 11, section 1), the offshore domain ischaracterized by the subduction of the South China Sea oceaniclithosphere under the PSP. The typical Manila oceanic accre-tionarywedge develops by accretion of the sediments deposited inthe Manila trench against the Luzon arc basement. Awide forearcbasin develops at the rear of the thrust wedge, mainly filled by arcsediments. This simple setting is the present-day analogue ofprocesses acting in the past more to the north, before thebeginning of the continental margin subduction. In our experi-ments, the first stages of accretionary wedge growth simulate theprocesses acting during oceanic subduction. During modelshortening the wedge growths by frontal accretion of small thrustunits. The step by step input of sand (sediments) in the back part ofthe developing wedge allows filling of a syntectonic basin (in aforearc setting), which development is controlled by tectonicwedging and backthrusting (Figs. 3–6, stages a, b). A recentsimilar interpretation is proposed by Chi et al. (2003), based onthe detailed analysis of seismic lines (Taicrust experiment) andgravity data.

2) Domain of incipient continental subduction.

The general map of Fig. 1 shows the main structural elementsand morphological units that characterize the deformation in thisdomain where a forearc basement sliver is proposed to besubducting beneath the PSP upper-plate. It reflects the complextectonic history suffered by the area. Six morphotectonicstructures constitute the domain of incipient continental subduc-tion: (1) The Kaoping Slope (KS), (2) the Hengchun Peninsula(HP) and its submarine equivalent the Hengchun Ridge (HR),(3) the Southern Longitudinal Trough (SLT) south of the on-landLongitudinal Valley (LV), (2) the elongated Huatung Ridge (HtR)forming the eastward dam of the Southern Longitudinal Trough,(3) the Taitung Trough (TT), marked by a sinuous V-shaped

valley, and (4) the Luzon volcanic arc including the islands ofLanyu and Lutao.

Offshore south of 22° N, the size, morphology and structure ofthe accretionary wedge change significantly owing to the firsteffects of the continental margin subduction (Fig. 9). The forearcbasin is shortened in between the rear of the wedge and thevolcanic edifice of the arc. Three morphotectonic units appear:—a lower-slope wedge with a very low dipping slope,— the HR isan uplifted domain of the wedge bounded by a slope break andcharacterized by a steeply dipping upper-slope, — the HtRsmaller ridge, composed by deformed strata of forearc sedimen-tary deposits, separated from the rear of the wedge by the TTnarrow north–south-oriented trough.

Different mechanical interpretations have been proposed forthese tectonic features. Reed et al. (1992) suggested significantshortening of the central domain of the wedge, with out-of-sequence thrusting at the boundary between upper and lowerslopes and major backthrusting in the forearc domain. Under-plating of thrust units in the core of the thrust wedge represents apossible cause for changes in the dip of the slope, the domain oflow dip slope representing the zone of frontal accretion, the highdip upper slope marking the area of underplating at depth (seealso experimental studies of Gutscher et al., 1998a, orKukowski et al., 2002). The smaller HtR has been interpretedas deformed sediments of the forearc basin (e.g. Malavieilleet al., 2002). In all the experiments (Figs. 3–7), the developmentof a topographic ridge against the low dip backstop marks theevolution of the sand wedge during the progressive retreat of thePVC plate. This confirms that in southern Taiwan, thesubduction of a forearc sliver in front of the arc edifice couldbe a good explanation for the growth of the Huatung Ridge eastof the accretionary prism.

North of 22° N, the HP represents the emerged continuation ofthe submarineHR (Fig. 9). At this latitude, a large part of the slopesediments from the continental margin is involved in theaccretionary wedge. Onland, the deformation structures ofsouthern Taiwan characterize the main tectonics events thatoccurred during the growth of the orogenic wedge. Thick series ofMiocene deposits in this area suffered low-grade metamorphism

Fig. 11. General interpretative sections showing the tectonic evolution of the orogenic wedge. Section 1, oceanic subduction and growth of a sedimentary wedge southof Taiwan; Section 2, incipient subduction of the continental margin and subduction of a slice of forearc basement inducing intense shortening of the forearcsedimentary units; Section 3, mature continental subduction and growth of the Taiwan orogenic wedge.


and ductile–brittle deformation during the Late Cenozoicorogeny. Most of the recent field investigations and structuralanalysis realized in this area (Chang et al., 2000, 2001; Lu et al.,2001; Chang et al., 2003) distinguish three main stages in thedeformation history that can be summarized as follows: (1) a first

stage involving an early west-vergent deformation and volumeloss resulting in thrusting, regional tilting of strata, slumping andsubsequent folding (early slumping being sometimes consideredas a first synsedimentary deformation phase, but as thisdeformation occurs during the growth of the accretionary


wedge, such structures were probably syntectonic of the firstphase); (2) a second stage being dominated by general shear,which resulted inwidespread east-vergent back-folding and back-thrusting associated with isoclinal folding; and (3) a third stagemainly involving transpression in association with E–W con-tractional thrusting and folding, as well as a new penetrativecleavage. Many of the well-characterized structures in the studyarea disappeared progressively towards the north as deformationbecomes more complex and as exhumation exposes more andmore deep rocks of the Central Range. The evolution of structuresin sandbox models suggests a possible scenario to account for thecomplex tectonic history of this area. Early structures of the firstphase (slumping, west vergent thrusting and folding) developsduring the forward growth of the marine accretionary wedge,before incoming of slopemargin sediments. As sedimentary inputdramatically increases with the approach of the continental slope,it will change the behaviour of the coulomb wedge. Such aphenomenon has similar consequences on wedge deformationand structures as incoming of asperities (ridges, seamounts,plateaus, area of rough basement with strong basal coupling…) ina critical wedge (see for example modeling of this process inLallemand et al., 1994; Dominguez et al., 1998a,b, 2000). Thus,change in the critical taper and subsequent thickening of thewedge occur inducing fault reactivations, out of sequencebackthrusting and associated backfolding. The structuresobserved onland attributed to a second tectonic stage couldreflect such event. As major consequence, strain and stressincrease induced in the thrust wedge could be responsible for the

Fig. 12. Oblique view (Digital Elevation Model) of the offshore domain SE of TaiwaLongitudinal Trough” orogenic basin.

strong deformation that affects the forearc domain, involvingsubduction of a slice of forearc basement (Fig. 11, section 2). Assubduction is oblique transpressive strain partitioning latelyconcentrates in this active area producing the E–W contractionalthrusting and folding that is attributed onland to a third tectonicevent (see orientation of fold axis in Fig. 9).

Malavieille et al. (2002) have shown that major shorteningoccurs today offshore in the forearc domain, between the LuzonArc (islands of Lutao and Lanyu) and the Hengchun Peninsulaof Taiwan. South of Taitung, the difference between GPS dataobtained on the arc islands (Lutao and Lanyu) and on east coastof the HP confirms that about 40 mm/yr (half of the totalconvergence) (Yu et al., 1997) is accommodated offshore. It ismainly absorbed by west-dipping thrusting beneath the HtR andin addition by folding and thrusting within the ridge (Fig. 10).The map (Fig. 9) and digital elevation model oblique view(Fig. 12) show that two main morphostructural units, the HtRand the SLT constitute the present forearc domain. Sections aand b of Fig. 10 show the geometry, deformation structures andtectonic setting of these units. The SLT is a proximal orogenicbasin developed in a forearc position (e.g., Lundberg andDorsey, 1988; Lundberg et al., 1997; Fuh et al., 1997).Elongated in a north–south direction between 21°50'N and22°40'N, it is bounded to the west by the 10°-east-dippingstructural slope of the HP and to the east, by an antiformalnarrow ridge which extends westward from the HR over-thrusting onto the Luzon arc near 22°05'N. The basin is filledby Holocene orogenic sediments coming from the Central

n Island suffering intense forearc shortening. Yellow color outline the “Southern

Fig. 13. Geological section of Fig. 10B interpreted at depth using the comparison with structures of a sandbox experiment. Subduction of a forearc basement slice wellaccounts for deformation, structures and basin geometry observed SE of Taiwan.


Range (Huang et al., 1992). Filling by growth strata record therelative uplift of the HR, forming a dam for sediments(Lundberg et al., 1992, 1997). Complex deformation andprogressive tilting of lower series have been imaged from east–west and north–south seismic lines (Lundberg et al., 1997;Malavieille et al., 2002). The upper series of the basin arerelatively flat, onlapping the HR to the south, whereas at depth,the lower strata overlying an irregular basement are gentlydeformed. These sequences lie unconformably on top of older,folded and faulted sequences of the former forearc basin. TheFig. 13 compares an evolved stage of a sand model to thegeological section (section a, Fig. 10) drawn using all availabledata. The interpretation proposed for the processes responsibleat depth for the observed structures is directly inspired by theexperiments. It summarizes the main characters of deformation(geometry and kinematics) and shows possible mechanismsable to produce the complex deformation suffered by the areaduring subduction of a forearc basement slice.

2) Domain of mature continental subduction and orogenicwedge growth.

From 22°40'N to about 24°N, the collision is completed andthe forearc domain is drastically reduced. This northern domainrepresents the area where the continental margin of China islargely involved in the subduction (Cheng et al., 2002). Thewedge growths again by frontal accretion to the west (e.g.,Simoës, 2005; Simoes et al., 2007), underplating in the centralpart of the belt (Beyssac et al., 2006), accretion of parts of the

arc-forearc domain, backthrusting and tectonic wedging in theeastern side of the orogenic belt to the east (Malavieille et al.,2002). The Coastal Range volcanic rocks and associated residualbasins are detached from the Philippine sea plate, overthrustingthe central Range to the west and backthrusting onto theHuatung Basin to the east. From Taitung to 23°40'N, 30 mm/yrof shortening are taken up today along the east-dipping thrusts ofthe Longitudinal Valley (e.g. Angelier et al., 1997), and about20 mm/yr through west-dipping thrusts located offshore close tothe base of the slope (Yu et al., 1997; Malavieille et al., 2002).The section 3 of Fig. 11 illustrates the deformation of the maintectonic units constituting the mature Taiwan belt, showing anevolved stage of processes acting today more to the south. In thisarea, the slice of forearc basement is completely subducted underthe PSP lithosphere. Such situation is equivalent to the maturestages of the experiments when the retreat of the intermediatePVC plate is completed. The wide orogenic wedge constitutedby all the various accreted units and growing foreland basin ispresently indented by the basement of the volcanic arc. Thetectonic history of this domain is described in Malavieille et al.(2002).

6. Conclusion

Most of the deformation and tectonic events recordedoffshore or onland in the complex area south of Taiwan canbe better explained using results of our specific modeling which


well describe the tectonic processes and basin developmentassociated with continental subduction under a volcanic arc.

To the south, incipient subduction of the continental margininduces increasing stress and strain in the upper plate. Subsequentsubduction of a forearc basement slice produces intense shorteningand concomitant deformation in the forearc domain. Such processinvolves deformation of the forearc basin previously developed ina setting of oceanic subduction. Volcaniclastic sediments of theforearc are involved in the growth of a new thrust ridgebackthrusted against the basement slope of the volcanic arcedifice.A syn-collisional orogenic basin develops which structuralevolution characterizes the progressive shortening of the forearcdomain. Thus, detrital sediments coming from the growingcontinental orogenic wedge are trapped in the piggy-back troughdeveloped between its backpart and the topographic high of thenew rising ridge.

North of the latitude of Taitung, the forearc basement of theLuzon volcanic arc no longer exists. The wedge growths again byfrontal accretion to the west, underplating in the central part of thebelt, accretion of parts of the arc–forearc domain, backthrusting andtectonic wedging in the eastern side of the orogenic belt to the east.Reconstruction of these processes may be useful for the under-standing of the early stages of mountain building in fossil orogens.

Acknowledgments

We thank “Institut National des Sciences de l'Univers”, theFrench Institute in Taipei (Ministry of Foreign Affairs), and theNational Science Council (Taiwan) for funding and supportingthis work. We thank S. Dominguez and E. Konstantinovskaia forstimulating discussion about experiments and C-Y. Lu and K-JChang for their geological help and kindness during our field tripsin Taiwan. Many thanks to A. Delplanque for helping draft mostof the figures in this paper. Critical reviews and comments byWei-Hau Wang and an anonymous reviewer are highlyappreciated. Figs. 1, 9 and 12, were produced using GMTsoftware (Wessel and Smith, 1995).

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http://dx.doi.org/10.1029/2002JB002274

http://dx.doi.org/10.1029/2002JB002274

http://dx.doi.org/10.1029/2004JB003251

http://dx.doi.org/10.1029/2006JB004824

http://dx.doi.org/10.1029/2002JB002190

consequences of continental subduction on forearc basin...

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