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Mawer (1988), Dynamic recrystallization <strong>and</strong>associated in perthites: Evidence <strong>of</strong> deep crustal thrusting, J. Geophys.Res., 93, 325–337, doi:10.1029/JB093iB01p00325.White, R. W., R. Powell, <strong>and</strong> T. J. B. Holl<strong>and</strong> (2001), Calculation <strong>of</strong> partialmelting equilibria in the system Na 2 O–CaO–K 2 O–FeO–MgO–Al 2 O 3 –SiO 2 –H 2 O (NCKFMASH), J. Metamorph. Geol., 19, 139–153, doi:10.1046/j.0263-4929.2000.00303.x.Závada, P., K. Schulmann, J. Konopásek, O. Lexa, <strong>and</strong> S. Ulrich (2007),Melt topology in deformed quartzo-feldspathic rocks: Implicationfor rheology <strong>and</strong> grain-scale migration <strong>of</strong> melt in partially molten crust,J. Geophys. Res., 112, B10210, doi:10.1029/2006JB004820.J. K. Becker, Institut für Geowissenschaften, Universität Tübingen,Sigwartstrasse 10, D-72076 Tübingen, Germany.O. Lexa, Institute <strong>of</strong> Petrology <strong>and</strong> Structural Geology, CharlesUniversity, Albertov 6, 12843 Praha 2, Czech Republic.J.-E. Martelat, Laboratoire de Géodynamique des Chaînes Alpines,UMR5025, Université Joseph Fourier, Observatoire des Sciences del’Univers de Grenoble, CNRS, F-38041 Grenoble Cedex 9, France.K. Schulmann <strong>and</strong> P. Štípská, Centre de Géochimie de la Surface,UMR7516, Université Louis Pasteur, CNRS, F-67084 Strasbourg Cedex,France.S. Ulrich, Geophysical Institute, Czech Academy <strong>of</strong> Sciences, Boční II/1401, 14131 Praha 4, Czech Republic.20 <strong>of</strong> 20314
J. metamorphic Geol., 2008, 26, 29–53 doi:10.1111/j.1525-1314.2007.00743.xOrigin <strong>of</strong> migmatites by deformation-enhanced melt infiltration<strong>of</strong> orthogneiss: a new model based on quantitativemicro<strong>structural</strong> analysisP. HASALOVÁ, 1,2 K. SCHULMANN, 1 O. LEXA, 1,2 P. ŠTÍPSKÁ, 1 F. HROUDA, 2,3 S. ULRICH, 2,4J. HALODA 5 AND P. TÝCOVÁ 51 Université Louis Pasteur, CGS/EOST, UMR 7517, 1 rue Blessig, Strasbourg 67084, France (hasalovap@seznam.cz)2 Institute <strong>of</strong> Petrology <strong>and</strong> Structural Geology, Charles University, Albertov 6, 12843 Prague, Czech Republic3 AGICO, Ječná 29a, 621 00 Brno, Czech Republic4 Institute <strong>of</strong> Geophysics, Czech Academy <strong>of</strong> Sciences, Boční II/1401, 14131 Praha 4, Czech Republic5 Czech Geological Survey, Klárov 3, 118 21 Prague 1, Czech RepublicABSTRACTA detailed field study reveals a gradual transition from high-grade solid-state b<strong>and</strong>ed orthogneiss viastromatic migmatite <strong>and</strong> schlieren migmatite to irregular, foliation-parallel bodies <strong>of</strong> nebulitic migmatitewithin the eastern part <strong>of</strong> the Gfo¨ hl Unit (Moldanubian domain, Bohemian Massif). The orthogneiss tonebulitic migmatite sequence is characterized by progressive destruction <strong>of</strong> well-equilibrated b<strong>and</strong>edmicrostructure by crystallization <strong>of</strong> new interstitial phases (Kfs, Pl <strong>and</strong> Qtz) along feldspar boundaries<strong>and</strong> by resorption <strong>of</strong> relict feldspar <strong>and</strong> biotite. The grain size <strong>of</strong> all felsic phases decreases continuously,whereas the population density <strong>of</strong> new phases increases. The new phases preferentially nucleate alonghigh-energy like–like boundaries causing the development <strong>of</strong> a regular distribution <strong>of</strong> individual phases.This evolutionary trend is accompanied by a decrease in grain shape preferred orientation <strong>of</strong> all felsicphases. To explain these data, a new petrogenetic model is proposed for the origin <strong>of</strong> felsic migmatites bymelt infiltration from an external source into b<strong>and</strong>ed orthogneiss during deformation. In this model,infiltrating melt passes pervasively along grain boundaries through the whole-rock volume <strong>and</strong> changescompletely its macro- <strong>and</strong> microscopic appearance. It is suggested that the individual migmatite typesrepresent different degrees <strong>of</strong> equilibration between the host rock <strong>and</strong> migrating melt duringexhumation. The melt topology mimicked by feldspar in b<strong>and</strong>ed orthogneiss forms elongate pocketsoriented at a high angle to the compositional b<strong>and</strong>ing, indicating that the melt distribution wascontrolled by the deformation <strong>of</strong> the solid framework. The microstructure exhibits features compatiblewith a combination <strong>of</strong> dislocation creep <strong>and</strong> grain boundary sliding deformation mechanisms. Themigmatite microstructures developed by granular flow accompanied by melt-enhanced diffusion <strong>and</strong>/ormelt flow. However, an AMS study <strong>and</strong> quartz micr<strong>of</strong>abrics suggest that the amount <strong>of</strong> melt present didnot exceed a critical threshold during the deformation to allow free movements <strong>of</strong> grains.Key words: crystal size distribution; melt infiltration; melt topology; migmatites; quantitative texturalanalysis.INTRODUCTIONMovement <strong>of</strong> a large volume <strong>of</strong> granitic melt is animportant factor in the compositional differentiation<strong>of</strong> the continental crust (Fyfe, 1973; Collins & Sawyer,1996; Brown & Rushmer, 2006) <strong>and</strong> the presence <strong>of</strong>melt in rocks pr<strong>of</strong>oundly influences their rheology(Arzi, 1978). The migration <strong>of</strong> melt through the crust iscontrolled by melt buoyancy <strong>and</strong> pressure gradientsresulting from the combination <strong>of</strong> gravity forces <strong>and</strong>deformation (Wickham, 1987; Sawyer, 1994). Thereare three major mechanisms controlling melt migrationthrough the continental crust: (i) diapirism resulting inupward motion <strong>of</strong> low-density magma through higherdensity rocks (Ch<strong>and</strong>rasekhar, 1961; Ramberg, 1981);(ii) dyking that describes melt migration by hydr<strong>of</strong>racturing<strong>of</strong> the host rock <strong>and</strong> transport <strong>of</strong> meltthrough narrow dykes (Lister & Kerr, 1991; Petford,1995); (iii) <strong>and</strong> migration <strong>of</strong> a melt through a network<strong>of</strong> interconnected pores during deformation or compaction<strong>of</strong> solid matrix (McKenzie, 1984; Wickham,1987).Brown & Solar (1998a) <strong>and</strong> Weinberg & Searle(1998) proposed that during active deformation meltmoves by pervasive flow <strong>and</strong> it is essentially pumpedthrough the system parallel to the principal finiteelongation in the form <strong>of</strong> foliation-parallel veins.Based on a number <strong>of</strong> field studies, pervasive meltmigration at outcrop scale controlled by regionaldeformation has been suggested by various authors(Collins & Sawyer, 1996; Brown & Solar, 1998b;V<strong>and</strong>erhaeghe, 1999; Marchildon & Brown, 2003).Ó 2007 Blackwell Publishing Ltd 29315
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