478 Int J Earth Sci (Geol Rundsch) (2012) 101:463–482significant viscosity contrasts exist between the basementand cover. In addition, it suggests that the absence <strong>of</strong> aweak detachment zone promotes infolding. The centralHearne domain may therefore represent a juvenile stage inthe evolution <strong>of</strong> cuspate infolding.In contrast to infolding <strong>of</strong> the cover and basement, somecover <strong>sequence</strong>s that contain upright folds are separatedfrom a penetratively deformed ductile basement by ashallow-dipping décollement. For example, in the SongpanGarzê fold belt <strong>of</strong> eastern Tibet upright buckle folds <strong>of</strong> aPalaeozoic sedimentary succession are separated from apenetratively deformed and locally migmatized granitoidbasement across a basal décollement <strong>of</strong> high-temperature,mid-pressure metamorphosed Devonian-Silurian slates(Calassou 1994; Xu et al. 1992; Roger et al. 2004; Harrowfieldand Wilson 2005). Folds in the cover <strong>sequence</strong>show axial planes orthogonal to the basal décollementwhere sheath folds indicate penetrative high shear strainductile <strong>deformation</strong> that also locally effects the basement(Roger et al. 2004: Harrowfield and Wilson 2005). Harrowfieldand Wilson (2005) suggest that this represents thetransition from a pure-shear dominated cover <strong>sequence</strong> to asimple-shear dominated ductile substrate. Models 61 and54 preserve a remarkably planar detachment between thedetachment zone (PDMS) and the underlying ductilesubstrate beneath upright folds in the cover <strong>sequence</strong>,analogous to the proposed development <strong>of</strong> the Songpan-Garzê fold belt (Harrowfield and Wilson 2005). This suggeststhe presence <strong>of</strong> a weak viscous detachment zone <strong>of</strong>sufficient thickness will promote a planar interface betweenthe basement and the overlying basal décollement andcover <strong>sequence</strong>.Detachment foldingDetachment folding has been extensively documentedwhen a competent <strong>sequence</strong> is folded over a less-viscousductile substrate (e.g. Costa and Vendville 2002). One <strong>of</strong>the best examples <strong>of</strong> detachment folding is found in theJura Mountains <strong>of</strong> Switzerland where a rigid basement isseparated from Mesozoic sediments by a Triassic evaporitelayer (Fig. 12a; Buxtorf 1916). Detachment folds have alsobeen documented in the Tian Shan region <strong>of</strong> the TibetanPlateau, where Indo-Asian convergence has deformedTertiary terrestrial sediments above a basal evaporativehorizon into box-like to upright isoclinal folds (Fig. 12b;Scharer et al. 2004). Structures akin to detachment folds ina <strong>layered</strong> sedimentary <strong>sequence</strong> develop when a layer <strong>of</strong>PDMS is present at the interface in our models (Fig. 12c).Detachment folding has been divided by Mitra (2003) intoFig. 12 Comparison <strong>of</strong> models to natural examples. a Detachmentfolds from the Jura mountains (modified from Mitra 2003 afterBuxtorf 1916). b Detachment folds from Tian Shan, China (modifiedfrom Scharer et al. 2004). c Detachment folds across the ductileinterface <strong>of</strong> Model 61. d Close-up photographs <strong>of</strong> the <strong>layered</strong><strong>sequence</strong> from Model 61 showing the transition from a disharmonicbox fold to a ‘lift-<strong>of</strong>f’ fold (Mitra 2003) e from stages A and B,respectively. f Lift-<strong>of</strong>f fold <strong>of</strong> the Weissenstein anticline in the Juramountains modified from Mitra (2003) after Buxtorf (1916)123
Int J Earth Sci (Geol Rundsch) (2012) 101:463–482 479two end members, suggested to represent the progressiveevolution <strong>of</strong> detachment folds: disharmonic detachmentfolds and lift-<strong>of</strong>f folds, based on the fold patterns observedin the Jura Mountains. Lift-<strong>of</strong>f folds have a parallelgeometry <strong>of</strong> the outer units and isoclinal folding <strong>of</strong> thedetachment between the upper <strong>sequence</strong> and less competentsubstrate in the core <strong>of</strong> the anticline where disharmonicfolds have a parallel geometry <strong>of</strong> the outer arc and nonparallelgeometries in the inner arc (Mitra 2003). Figure 12shows close-up photographs <strong>of</strong> Model 61 and the evolutionfrom a box fold (Fig. 12d) into a lift-<strong>of</strong>f structure(Fig. 12e) compared with the Weissenstein anticline fromthe Jura Mountains (Fig. 12f). Mitra (2003) predicts thatincreased bulk shortening will progressively produce openbroadfolds, then disharmonic folds, and finally lift-<strong>of</strong>ffolds. No single fold depicts all these stages, but examples<strong>of</strong> all <strong>of</strong> these stages in Model 61 support the <strong>sequence</strong> <strong>of</strong>detachment fold formation proposed by Mitra (2003).Conclusions<strong>Centrifuge</strong> analogue models display features that simulatethe development <strong>of</strong> first-order active folds in ductile layerswhere (1) a metamorphic basement and an overlying sedimentarycarapace constituting a sedimentary superstructureand metamorphic infrastructure is deformed throughlayer-parallel shortening in large hot orogens and in someArchaean granite-greenstone belts and (2) structures duringactive folding (in the absence <strong>of</strong> faulting) <strong>of</strong> a <strong>layered</strong>sedimentary <strong>sequence</strong> upon a thick ductile substrate in foldbelts. CT scanning <strong>of</strong> models using newly developedtechniques and materials has proven to be an excellentmeans to examine the 4D development <strong>of</strong> structures withinmodels that has not been possible in previous studies.Viscosity contrasts across the basal décollement controlif detachment folding develops above a flat interface or ifinfolding dominates the cover–basement geometry. A weakbasal décollement promotes detachment folding, whereas arelatively stronger detachment promotes infolding. A weakdetachment also promotes a broad and open fold train incontrast to a more irregular <strong>sequence</strong> <strong>of</strong> folds above a moreviscous ductile substrate. Contrary to sandbox models,whilst folds may differ, no consistent curvature <strong>of</strong> fold axesacross the interface <strong>of</strong> a more ductile décollement isobserved.A <strong>layered</strong> <strong>sequence</strong> with thicker individual layers promotesa regular upright fold train with a consistent foldamplitude and wavelength during bulk shortening, whereasthinner individual layers show a more irregular fold distributionwith a greater variety <strong>of</strong> fold styles, vergences,amplitudes, and wavelengths. Folds above a weak ductiledécollement display either a slight hinterland vergence orno discernable preferred fold asymmetry. A stronger basaldécollement promotes foreland-verging folds. Cuspatestructures can develop within a weak horizon bounded bytwo stronger horizons and evolve from open and upright, totighter and angular, and finally through lateral materialmigration from the limbs into the hinges <strong>of</strong> individualfolds. Folds <strong>of</strong> a competent horizon within the basal ductilesubstrate differ and may be out <strong>of</strong> phase with folds in thecover <strong>sequence</strong>.Acknowledgments Acknowledgment is made to the Donors <strong>of</strong> theAmerican Chemical Society Petroleum Research Fund for funding CTscanning and centrifuge <strong>modelling</strong> research at INRS-ETE and toNSERC for Discovery grants to L. Harris and L. Godin. Modellingwas undertaken by C. Yakymchuk whilst recipient <strong>of</strong> an NSERCUSRA Summer Research Scholarship. The laboratory for physical,numerical, and geophysical simulations at INRS-ETE was funded byCFI and MELS-Q grants to L. Harris with contributions from INRS-ETE, Applied Geodynamics Laboratory <strong>of</strong> the Bureau <strong>of</strong> EconomicGeology (University <strong>of</strong> Texas at Austin, who donated the centrifuge),Sun Microsystems, Seismic Microtechnology, and Norsar. CT scanningwas undertaken by L.-F. Daigle in the Quebec MultidisciplinaryScanography Laboratory at INRS-ETE. Effective viscosity measurementswere undertaken by J. Poulin and E. Konstantinovskaya;M. Bousmina, Département génie des mines, métallurgie et matériaux,Universté Laval, is thanked for access to his polymer rheologylaboratory and M. Rousseau for instruction and assistance in viscositymeasurements. S. Cruden is thanked for providing PDMS andB. Giroux for allowing LH workstation access for 3D visualization <strong>of</strong>CT scans. CY thanks the Battertons for their hospitality for theduration <strong>of</strong> the <strong>modelling</strong> program. Careful reviews by C. Dietl andan anonymous reviewer and editorial handling by R. Greiling helpedus substantially improve this manuscript.ReferencesAffolter T, Gratier J-P (2004) Map view retro<strong>deformation</strong> <strong>of</strong> anarcuate fold-and-thrust belt: The Jura case. 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