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Journal of Petrology 2004 45(7):1393-1412; doi:10.1093/petrology/egh017
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Journal of Petrology 45(7) © Oxford University Press 2004; all rights reserved

Metapelites of the Kanskiy Granulite Complex (Eastern Siberia): Kinked PT Paths and Geodynamic Model

TARAS V. GERYA1,2,* and WALTER V. MARESCH2

1 INSTITUTE OF EXPERIMENTAL MINERALOGY, RUSSIAN ACADEMY OF SCIENCES, CHERNOGOLOVKA, MOSCOW DISTRICT, 142432, RUSSIA
2 INSTITUT FÜR GEOLOGIE, MINERALOGIE UND GEOPHYSIK, RUHR-UNIVERSITÄT BOCHUM, UNIVERSITÄTSTRASSE 150, 44780 BOCHUM, GERMANY

RECEIVED NOVEMBER 15, 2002; ACCEPTED JANUARY 1, 2003


    ABSTRACT
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
The Southern Yenisey Range (Eastern Siberia) consists of the granulite-facies Kanskiy complex bordered by the lower-grade Yeniseyskiy and Yukseevskiy complexes. Samples of metapelite of the Kanskiy complex typically show characteristic garnet-forming reaction textures and near-isobaric cooling PT paths. An important new result of this study concerns the difference in shape of the PT paths from different parts of the Kanskiy granulite complex: metapelites collected ~8 km from the boundary with the Yeniseyskiy complex followed a linear path with dP/dT {approx} 0·006 kbar/°C; metapelites collected ~3 km from this boundary reveal a kinked PT path with an interval of burial cooling (dP/dT {approx} –0·006 kbar/°C). The difference in the shape of the PT paths is supported by the chemical zoning of garnet studied in the second group of samples. A mechanism of buoyant exhumation of granulite is suggested by comparison with the results of numerical modelling, which indicate that such a diversity of PT paths may result from a transient disturbance of the thermal structure by rapid differential movement of material from different crustal levels. To arrive at a correct tectonic interpretation, the whole assemblage of interrelated PT paths of metamorphic rocks collected from different localities within the same complex must be studied.

KEY WORDS: crustal diapirism; exhumation; granulites; numerical modelling; PT path


    INTRODUCTION
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
This paper addresses the petrology and PT history of metapelitic gneisses of the Kanskiy granulite complex in the Southern Yenisey Range (Eastern Siberia). Numerical modelling of these data allows the exhumation history of this high-grade terrain to be constrained.

Recent studies of Precambrian high-grade granulite complexes and adjacent lower-grade cratonic granite–greenstone terrains in Southern Africa and Russia suggest that both low- and high-grade metamorphic rocks from these areas record evidence for the metamorphic and tectonic events leading to the thrusting of granulites onto the adjacent granite–greenstone terrains (e.g. Perchuk, 1989Go; Van Reenen et al., 1990Go; Roering et al., 1992aGo, 1992bGo; Mints et al., 1996Go; Perchuk et al., 1996Go, 1999Go, 2000aGo, 2000bGo; Pozhilenko et al., 1997Go; Perchuk & Krotov, 1998Go). In Southern Africa (the Southern Marginal Zone of the Limpopo complex) and in the Kola Peninsula (the Lapland complex) regional, crustal-scale shear zones separate the granulite terrains from the lower-grade granite–greenstone terrains. The emplacement of relatively hot, ductile granulites onto relatively cold, brittle cratonic successions caused heat transfer from the exhuming granulites to the underlying wall rocks, resulting in the development of dynamic polythermal–polybaric metamorphic zoning (Roering et al., 1992aGo; Perchuk et al., 1996Go; Perchuk & Krotov, 1998Go).

Published data (e.g. Kusnetsov, 1941Go, 1988Go; Kovrigina, 1973Go, 1977Go; Nozkhin, 1983Go, 1985Go; Gerya et al., 1986Go; Perchuk et al., 1989Go; Dacenko, 1995Go) suggest that the Southern Yenisey Range of Eastern Siberia is composed of metamorphic complexes of different metamorphic grade separated by regional thrusts (Fig. 1). The degree of metamorphism generally increases across the thrust system from greenschist- and epidote–amphibolite-facies conditions (the Yukseevskiy complex) through amphibolite-facies (the Yeniseyskiy complex) to granulite-facies conditions (the Kanskiy complex) (e.g. Kusnetsov, 1941Go, 1988Go; Gerya et al., 1986Go; Perchuk et al., 1989Go). Recent combined structural and petrological studies (Smit et al., 2000Go) suggest that all three complexes are characterized by a uniform D2 shear pattern that was formed during the exhumation of the Kanskiy complex.



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Fig. 1. Regional position (a) and geological structure (b) of the Southern Yenisey Range, Eastern Siberia. (a) Main geological units of the Yenisey Range. 1, cover rocks; 2–4, Pre-Riphean metamorphic complexes: 2, Kanskiy and Yeniseyskiy granulitic–gneissic complexes, amphibolite- to granulite-facies metamorphism (>1900 Ma); 3, Yukseevskiy greenstone complex, greenschists to epidote–amphibolite-facies metamorphism (>1900 Ma); 4, Teyskiy complex (gneisses, carbonate rocks, quartzites, micaceous schists, metabasites), greenschist- to amphibolite-facies metamorphism (>1650 Ma); 5, Riphean volcanic and sedimentary complexes; 6, Lower Proterozoic granitoids; 7, Upper Proterozoic granitoids; 8, geological boundaries; 9, thrusts. (b) Geological map of the Southern Yenisey Range. Major regional thrust systems: I, Pri-Yeniseyskiy; II, Kansko-Posolnenskiy; III, Kansko-Shilkinskiy. Circles with numbers show the location of samples listed in Table 1: 1—A257, A-256, A-258, A-260, A-269, A-271, A-275; 2—A-538, A-643, A-720. A, B, C, E and F are specific localities referred to in the text.

 
Smit et al. (2000)Go suggested that both the tectono-metamorphic pattern and the evolution of the metamorphic complexes of the Southern Yenisey Range are very similar to those described for the c. 2600 Ma Limpopo complex of Southern Africa and the c. 1900 Ma Lapland complex of the Kola Peninsula. Similar geodynamic processes therefore appear to be responsible for the formation of these high-grade terrains. Similarities in the reaction textures of granulites in all three metamorphic terrains have also been recognized (Perchuk et al., 2000b)Go. However, in both the Limpopo and Lapland complexes, metapelitic granulites show characteristic garnet-forming reaction textures that can be related to a distinctively kinked retrograde PT path (Fig. 2) with an intermediate near-isobaric cooling interval (dP/dT = 0·007–0·008 kbar/°C, Perchuk et al., 2000bGo; Smit et al., 2001Go). Such PT paths have so far not been described for the Kanskiy granulite complex (Perchuk et al., 1989Go).



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Fig. 2. Typical examples of kinked PT paths in metapelites of the Limpopo and the Lapland granulite complexes, as inferred from mineral zoning and reaction textures (Perchuk et al., 2000bGo; Smit et al., 2001Go).

 
In this paper we present the first evidence that kinked retrograde PT paths are also found in metapelitic granulites sampled close (~3 km) to the border of the Kanskiy granulite complex, allowing us to discuss the geodynamic significance of this phenomenon.


    GEOLOGICAL SETTING
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
The Yenisey Range is situated in the major Baikalide belt that subdivides Siberia into Western and Eastern Platforms (Fig. 1). The Baikalide belt occurs as a semi-circular rim around the Eastern Siberian Platform that, among other geological features, also hosts the Yenisey Range (Fig. 1a). The Yenisey Range is about 700 km in length and 150 km wide and consists of metamorphic, magmatic and sedimentary complexes of Archaean to Cenozoic age (Fig. 1a). The Southern Yenisey Range (Fig. 1b) constitutes a Precambrian metamorphic terrain with an exposed outcrop length of about 200 km and a width of 50–70 km. The regional structural framework of the Southern Yenisey Range has been traditionally interpreted as a system of north–south- to NW–SE-oriented crustal blocks (e.g. Kovrigina, 1973Go, 1977Go; Dacenko, 1995Go). On the basis of metamorphic, petrological and geochemical evidence, a subdivision into the Kanskiy, Yeniseyskiy and Yukseevskiy complexes has been recommended (Kusnetsov, 1941Go, 1988Go; Nozkhin, 1983Go, 1985Go; Gerya et al., 1986Go; Perchuk et al., 1989Go). These blocks are characterized internally by large-scale (100–800 m) isoclinal folds with axial planes dipping to the NE, well-developed lineations and a regional schistosity. Thrusts in the area follow the general structural trend of the Range and three major regional thrust systems are distinguished from west to east (Fig. 1b): the Pri-Yeniseyskiy, Kansko-Posolnenskiy and Kansko-Shilkinskiy thrusts (Kovrigina, 1973Go). Their orientation changes from NW–SE in the south to north–south in the north, following the contours of the Siberian Craton. The thrust systems, which dip at 50–70°E to the NE, with a general vergence towards the west, are composed of up to 4 km wide zones of mylonitization and are characterized by the presence of magmatic complexes and hydrothermal ore deposits. This uniform structural pattern across the Southern Yenisey Range has been traditionally attributed to folding during the systematic accretion of the Kanskiy, Yeniseyskiy and Yukseevskiy metamorphic complexes onto the western boundary of the Eastern Siberian Craton (e.g. Dacenko, 1995Go). Recently, however, Smit et al. (2000)Go studied the structural–metamorphic evolution of the Kanskiy, Yeniseyskiy and Yukseevskiy complexes of the Southern Yenisey Range along the Yenisey River section (Fig. 1). Three deformational events were recognized in each of the three complexes: a D1 fabric-forming event, a D2 shear and folding event, and a D3 shear event. Thrust kinematics across the Southern Yenisey Range suggest that during the D2 event the Kanskiy complex was thrust along a regional ductile shear zone onto the lower-grade complexes. This resulted in shearing and folding as well as the development of a dynamic metamorphic zonation.

The major stage of granulite-facies metamorphism in the Kanskiy complex was dated at 1800–2000 Ma, based on the zircon studies of Nozkhin et al. (1989)Go and Bibikova et al. (1993)Go. This age correlates well with the 1900 ± 100 Ma emplacement age of the Tarakskiy granites (Gerling & Artemov, 1964Go; Volobuev et al., 1976Go). An early thermal event is indicated for the period 2650 ± 50 Ma (Nozkhin et al., 1989Go; Bibikova et al., 1993Go), but the age of the protolith must exceed 2700 Ma. The major stage of epidote–amphibolite- to amphibolite-facies metamorphism in the Yeniseyskiy complex (1850 ± 150 Ma, Nozkhin et al., 1989Go; 1900–1860 Ma, Bibikova et al., 1993Go) correlates with the main granulite-facies event in the Kanskiy complex. A wide range of zircon ages have been determined for the rocks of the Yukseevskiy complex (Nozkhin et al., 1989Go; Nozkhin, 1997Go): 2750 Ma, 1900 Ma, 1450 Ma, 1050 Ma, 870 Ma and 600 Ma. Nozkhin et al. (1989)Go interpreted the 2750 Ma age as the time of formation of the volcano-sedimentary protolith of the Yukseevskiy complex and the 1450 Ma stage as the time of formation of the regional sub-meridional tectonic structure (Fig. 1a) of the entire Yenisey Range (Nozkhin et al., 1989Go). The three youngest ages correlate with the intrusion of Upper Proterozoic granites into the Kanskiy complex (Volobuev et al., 1976Go, 1980Go; Dacenko, 1984Go; Nozkhin et al., 1989Go).

Although the geochronology of the area is thus based on a very limited database, it does indicate that important metamorphic events occurred during the period 1800–2000 Ma in all three complexes of the Southern Yenisey Range. This period corresponds to the peak of the thermal activity in the area and to the formation of the Tarakskiy granitoid batholith during the final stages of granulite-facies metamorphism. According to the interpretation of Smit et al. (2000)Go, the major D2 stage of the metamorphism in all three complexes in the period 2000–1800 Ma corresponds to deformation and heat transfer caused by the exhumation of the Kanskiy complex. The D3 mylonitization event, on the other hand, was related to the formation of large-scale mylonitic shear zones (Fig. 1a and b) that occur across the entire Yenisey Range, dated at 1450 Ma by Nozkhin et al. (1989)Go.


    GEOLOGY OF THE KANSKIY GRANULITE COMPLEX
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
The Kanskiy granulite complex is subdivided into a lower Kuseevskiy and an upper Atamanovskiy sequence (Fig. 1b). The Kuseevskiy sequence is mainly composed of garnet–plagioclase, garnet–orthopyroxene–plagioclase and orthopyroxene–plagioclase gneisses and granulites, orthopyroxene–spinel–plagioclase ± garnet metabasites, aluminous metapelites with garnet, cordierite, sillimanite, spinel and orthopyroxene, as well as some charnockites and enderbites. The sequence also contains several metagabbro massifs of the Zimoveyninskiy complex (Fig. 1b). The assemblage quartz + orthopyroxene + sillimanite that characterizes peak (T ~900°C and P ~8 kbar) metamorphic conditions is found in some metapelites of the sequence (Perchuk et al., 1989Go). Maximum PT conditions recorded in garnet–cordierite–sillimanite–quartz metapelites correspond to 795°C and 6·1 kbar (Perchuk et al., 1989Go).

The Atamanovskiy sequence consists of aluminous garnet–biotite, garnet–cordierite–biotite, garnet–cordierite–sillimanite–spinel–two-feldspar metapelites, orthopyroxene–garnet–biotite, orthopyroxene–biotite–cordierite and orthopyroxene–plagioclase gneisses and rare orthopyroxene–spinel–plagioclase metabasites. The assemblage quartz + orthopyroxene + sillimanite is not found in metapelites of the sequence and the maximum PT conditions recorded in garnet–cordierite–sillimanite–quartz metapelites are 716°C and 4·5 kbar (Perchuk et al., 1989Go). In the NE part of the area near the Tarakskiy pluton (locality E in Fig. 1b) some metapelites of the Atamanovskiy sequence contain andalusite (Serenko, 1969Go; Perchuk et al., 1989Go). The intensively migmatized northeastern portion of the sequence demonstrates a gradual transition into granites of the Tarakskiy pluton (Dacenko, 1984Go).

Metapelites from both sequences of the Kanskiy complex show near-isobaric cooling reaction textures such as replacement of cordierite by garnet, sillimanite and quartz (Perchuk et al., 1989Go). These textures are more characteristic for metapelites taken from areas farthest from the Tarakskiy pluton and closest to the contacts between the Kanskiy and the Yeniseyskiy complexes (localities A, B and C in Fig. 1b) (Perchuk et al., 1989Go). In the western part of the area close to the Yenisey river this contact is also marked by the appearance of orthopyroxene + sillimanite in metapelites (e.g. localities A and B in Fig. 1b) and orthopyroxene + spinel + garnet + plagioclase in metabasites (e.g. localities A, B and F in Fig. 1b) of the Kuseevskiy sequence (Serenko, 1969Go; Perchuk et al., 1989Go).

Despite their high-grade character, the major rock types of the Kanskiy complex are geochemically very similar to typical Archaean granite–greenstone complexes (Nozkhin & Turkina, 1993Go): the garnet–orthopyroxene–biotite gneisses are analogous to volcanic rocks of andesitic and dacitic composition, whereas the aluminous gneisses are similar to pelitic rocks. The orthopyroxene–spinel–plagioclase metabasites demonstrate characteristics of tholeiitic basalts. The average chemical composition of the Kanskiy complex corresponds to granodiorite (Nozkhin & Turkina, 1993Go). An increase in the relative amount of mafic rocks in a northwesterly direction within the Kanskiy complex was described by Nozkhin & Turkina (1993)Go. The most significant amount of granulite-grade metabasic rock is concentrated along the Yenisey River, including the 1·5 km x 25 km layered Zimoveyninskiy metagabbro massif (Fig. 1b).


    MINERALOGY AND PETROLOGY OF STUDIED SAMPLES
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
For petrological study we selected 11 samples of metapelite containing the assemblage garnet + cordierite + sillimanite + quartz + K-feldspar + plagioclase + biotite collected from the rocks of the Atamanovskiy sequence from two localities at different distances (~3 km and ~8 km, see Fig. 1) from the boundary with the Yeniseyskiy complex. Mineral assemblages and bulk chemical compositions of these samples are listed in Tables 1 and 2, respectively. Microprobe analyses of coexisting minerals from these samples were carried out using the CamScan scanning electron microscope equipped with EDS Link AN10/85S at the Department of Petrology, Moscow State University, as well as the Cameca electron microprobe analyzer of the Institute of Experimental Mineralogy, Russian Academy of Sciences. Selected microprobe analyses of studied minerals are given in the Electronic Appendix to this paper, which may be downloaded from the Journal of Petrology website at http://www.petrology.oupjournals.org/.


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Table 1: Mineral assemblages of metapelites studied

 

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Table 2: Bulk chemical compositions* of metapelites studied

 
The fabric of the metapelites is dominated by porphyroblasts of garnet and cordierite set in a matrix of sillimanite, quartz, K-feldspar, plagioclase and biotite (Figs 3 and 4). As will be shown below, these garnet and cordierite compositions reflect PT conditions close to peak metamorphism and early stages of cooling. They will be referred to as Grt1 and Crd1 in the following discussion. Early generation Grt1 is represented by large (3–10 mm) isometric poikiloblasts containing abundant quartz and biotite inclusions (Fig. 3a, c and d). First generation Crd1 also forms large (1–3 mm) isometric, inclusion-rich poikiloblastic grains (Fig. 3b) or aggregates. In both localities studied, Crd1 contains conspicuous spinel + quartz symplectites (Fig. 4a and b) formed by decomposition of the cordierite according to the reaction

(1)
presumably at some early stage of the high-temperature history of the rock.



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Fig. 3. Back-scattered electron images of early garnet (Grt1) (a, c, d) and cordierite (Crd1) (b) porphyroblasts in samples studied.

 


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Fig. 4. Typical examples of reaction textures. (a, b) Replacement of cordierite by spinel + quartz intergrowths in samples A-275 (a) and A-538 (b). (c) Replacement of biotite by cordierite and orthopyroxene in sample A-538. (d) K-feldspar aureoles formed at the contact between garnet and quartz in sample A-538.

 
A second, younger generation of garnet (Grt2) is found in thin (≤0·2 mm) garnet–sillimanite–quartz intergrowths formed at the contact between the early poikiloblastic garnet with early cordierite (Fig. 5). Small (≤0·1 mm) idioblastic crystals of garnet are characteristic of this reaction texture (Fig. 6). The intergrowths can be interpreted as forming by decomposition of cordierite according to the reaction

(2)
Similar intergrowths have been described from the Limpopo and the Lapland granulite-facies terrains (Perchuk et al., 1996Go, 2000bGo; Smit et al., 2001Go).



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Fig. 5. Back-scattered electron images of later garnet (Grt2) and garnet + sillimanite + quartz intergrowths replacing cordierite in samples studied.

 


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Fig. 6. Back-scattered electron images (a, c) and chemical zoning patterns (b, d) of newly formed idioblastic garnet (Grt2) in samples studied.

 
The designation Crd2 is used here for non-porphyroblastic cordierite in medium- to fine-grained intergrowth with Grt2, sillimanite, biotite, plagioclase and quartz (Figs 5 and 6). Because of the small grain size, these crystals have equilibrated with Grt2 during the cooling history of the rock.

In sample A-538 (Table 1) specific reaction textures occur involving biotite and K-feldspar (Fig. 4c and d). In this sample, biotite grains and biotite–sillimanite intergrowths are commonly replaced by cordierite and orthopyroxene (Fig. 6c) without the formation of other potassium-bearing phases. This suggests dehydration reactions, with associated loss of the potassium component into the melt or metamorphic fluid, caused either by a temperature rise or a decrease in water activity. On the other hand, inclusions of quartz in early poikiloblastic garnet (Grt1) are commonly surrounded by K-feldspar microveins (Fig. 4d). Similar reaction textures related to the charnockitization process have been described in granulites from several regions and reflect mobility of potassium in the presence of either metamorphic fluid or partial melt during granulite-facies metamorphism (e.g. Perchuk & Gerya, 1992Go, 1993Go; Perchuk et al., 1994Go, 2000cGo; Newton, 1995Go).

Figures 68 show typical zoning profiles of coexisting garnet and cordierite of different generations. It is seen that both Crd1 and Crd2 are characterized by a significant increase in Mg content from the core [XMg = 0·6–0·7, where XMg = Mg/(Mg + Fe)] toward the rim (XMg = 0·75–0·8), particularly in contact with garnet. Chemical zoning of garnet is different in samples from the two localities. Early poikiloblastic garnet (Grt1) from sample A-275 collected close to the boundary of the Kanskiy complex in several cases demonstrates a notable decrease in Mg content from the core (XMg = 0·19–0·21) to the rim (XMg = 0·16–0·17, Fig. 7b), whereas similar garnet in samples A-538 and A-643 collected further away from this boundary is characterized by relatively constant Mg contents (XMg = 0·23–0·25, Fig. 8a and b). Second generation garnet (Grt2) in all samples commonly shows an increase in Mg content (XMg = 0·23–0·24 in the core, XMg = 0·26–0·31 in the rim) toward the contact with cordierite. This is observed for both younger idioblastic Grt2 grains (Fig. 6b and d) and in garnet + sillimanite + quartz intergrowths surrounding Grt1 porphyroblasts (Figs 7a, b, and 8a, b), and is especially characteristic for samples collected close to the contact of the Kanskiy granulite complex with the Yeniseyskiy complex.



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Fig. 7. Typical chemical zoning profiles for contacting porphyroblasts of early garnet (Grt1) and cordierite (Crd1) for samples A-258 (a) and A-275 (b), (c) collected ~3 km from the boundary of the Kanskiy complex.

 


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Fig. 8. Typical chemical zoning profiles for contacting porphyroblasts of early garnet (Grt1) and cordierite (Crd1) for samples A-643 (a) and A-538 (b, c) collected ~8 km from the boundary of the Kanskiy complex.

 

    THERMOBAROMETRY AND PT PATHS
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
Methods
Thermobarometry of granulites is recognized as a complex problem that cannot be solved only by the simple routine methods applicable to lower-grade metamorphic rocks (e.g. Frost & Chacko, 1989Go; Spear & Florence, 1992Go; Spear, 1993Go). Frost & Chacko (1989)Go concluded that special care must be taken to maximize the chance of correct retrieval of peak metamorphic conditions and accurate retrograde PT paths for granulites. One of the most crucial criteria is the interpretation of reaction textures to test and corroborate the PT trajectories obtained on the basis of thermobarometry alone (e.g. Frost & Chacko, 1989Go; Harley, 1989Go).

The approach and methods adopted here have been discussed and validated at length by Smit et al. (2001)Go. Critical aspects are the assumption that the cores of large grains can remain unaffected by later diffusion, whereas the rims reflect re-equilibration. Because reaction (2) leads to armouring of garnet and cordierite by quartz–sillimanite intergrowths, late Fe, Mg exchange in these reaction zones is arrested and intermediate stages of the cooling trajectory can be monitored. In addition, the net transfer reactions implied by specific PT trajectories must be corroborated by modal changes, i.e. reaction textures, in the rock.

Another important aspect is the corroboration of a PT trajectory via the pattern of chemical zoning of the minerals involved in the net transfer and exchange reactions. Inferred changes in dP/dT along the PT trajectory should be reflected in corresponding changes in the chemical zoning patterns of these minerals. This qualitative and relative test reflects discontinuities in trend vectors and does not depend directly on the absolute accuracy of individual PT estimates defined by uncertainties in both the analytical and thermodynamic data used.

For thermobarometric calculations we used the internally consistent thermodynamic dataset of Perchuk et al. (1985)Go and Perchuk (1990)Go, which is calibrated on the basis of experimental data on mineral equilibria involving solid solutions of garnet, orthopyroxene and cordierite (Perchuk & Lavrent'eva, 1983Go; Aranovich & Podlesskii, 1989Go). However, the results obtained are not specific to this dataset. Similar conclusions can be reached with the use of other datasets such as that of Holland & Powell (1998)Go, applicable to the calculation of phase diagrams for cordierite-bearing granulites (e.g. Gerya et al., 2001Go). The procedure followed to derive realistic PT paths involves the following four major steps [see Perchuk et al. (1996Go, 2000bGo) and Smit et al. (2001)Go, for further elaboration as well as details on calculations and worked examples].

  1. The sequence of events responsible for the formation of minerals and observed reaction textures is established.
  2. The chemical evolution of rock-forming minerals is determined by detailed microprobe profiling, allowing the distinction between exchange (diffusion) and net-transfer (mineral growth/decomposition) reaction mechanisms.
  3. Specific PT coordinates are calculated for the different stages of formation of mineral assemblages using the ‘core–core -> rim–rim’ method for each given generation of minerals. Representative rim compositions are selected on the basis of microprobe profiling to avoid the influence of later exchange diffusion on thermobarometry (e.g. Frost & Chacko, 1989Go; Spear & Florence, 1992Go). Equilibrium compositions of cores are assumed for relatively large (>1 mm) mineral grains that show chemical profiles with a central plateau of constant composition (e.g. Spear & Florence, 1992Go). Temperatures are calculated (Table 3) using garnet–cordierite pairs (Perchuk and Lavrent'eva, 1983Go) and pressures obtained from garnet–sillimanite–cordierite–quartz (Perchuk et al., 1985Go, 2000bGo).
  4. A PT trajectory is derived on the basis of individually calculated PT points. The consistency of the PT trajectory is tested with both mineral zoning (i.e. the relationship between the PT path vector and the array of calculated compositional isopleths in observed divariant assemblages) and the observed reaction textures. For the latter, we relate the PT path to isopleths of relative garnet mode in the observed divariant assemblages (Gerya, 1991Go; Perchuk et al., 2000bGo; Smit et al., 2001Go). The isopleths of relative garnet mode, representing the atomic ratio 100(Mg + Fe)in garnet/(Mg + Fe)in rock, are calculated by solving a system of thermodynamic and mass balance equations for the observed cordierite + garnet + sillimanite + quartz assemblage on the basis of the bulk-rock compositions given in Table 2 [see Perchuk et al. (2000b)Go and Smit et al. (2001)Go for details of the method of calculation]. By comparing the PT path with the isopleths of relative garnet mode it can be inferred whether garnet should grow or decompose along a specific section of this path, a conclusion that can in turn be tested by reaction textures studied in the sample. The calculation of isopleths of relative garnet mode assumes complete re-equilibration of a rock with changing PT parameters, which is not realized in most cases. Therefore the comparison with PT paths obtained by thermobarometry is a qualitative test.


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Table 3: Selected P–T coordinates of garnet–cordierite–sillimanite–quartz equilibria for samples from Table 1

 
Thermodynamic calculations for the divariant assemblage Grt + Sil + Crd + Qtz were carried out using internally consistent thermodynamic data (Perchuk et al., 1985Go) for the reactions

and

Activities of the solid-solution end-members were calculated as follows (Perchuk et al., 1985Go; Gerya & Perchuk, 1990Go):

where W = –1333 + 0·617T – 0·336P + 1026(1 – XH2O) + 472(1 – XH2O)2, XMg = Mg/(Fe + Mg); XFe = Fe/(Fe + Mg); XH2O = H2O/(H2O + CO2) is the mole fraction of water in the metamorphic fluid.

We believe that the systematic application of the above procedure allows the derivation of a PT path that is consistent with both mineral zoning and reaction textures, and, therefore, has a very good chance of closely approximating the actual PT trajectory of the rock. The accuracy of individual PT coordinates calculated along this trajectory depends on the uncertainties in both the analytical and thermodynamic data involved. For the present study this accuracy can be estimated to be ±30°C and ±0·5 kbar (Perchuk et al., 1985Go; Perchuk, 1990Go). To minimize the influence of the thermodynamic uncertainties on our results we used the same set of geothermometers and geobarometers for all studied samples. This allows accurate relative comparison of the geometry of PT paths inferred for different samples on the basis of different patterns of garnet and cordierite zoning (see Figs 5, 7 and 8).

Results
Figures 912 show the results of thermobarometry and PT paths derived from reaction textures and mineral zoning. Selected compositions of coexisting garnet and cordierite and the resulting PT estimates are listed in Table 3. The PT paths for samples from the two studied localities are distinctly different. For samples collected far from the boundary of the Kanskiy complex (locality 2), essentially linear, near-isobaric cooling PT trajectories (dP/dT = 0·005–0·006 kbar/°C) are characteristic. On the other hand, samples collected close to this boundary demonstrate kinked PT paths with an intermediate interval of burial cooling (i.e. cooling at increasing pressure) with negative dP/dT slope (–0·005 to –0·006 kbar/°C). Figures 9c12c show the results of thermodynamic modelling of XMg of garnet and cordierite coexisting along the PT paths. These results are consistent with the observed chemical zoning (compare Figs 6 8 and 9c12c). Figures 9d12d represent the equilibrium relative modal amounts of garnet calculated along the PT paths using the bulk compositions of the rocks studied (Table 2). As can be seen, an intensive growth of newly formed garnet and garnet–sillimanite–quartz intergrowths replacing cordierite is consistent with conditions of near-isobaric cooling. In particular, the burial cooling stage of samples A-258 and A-275 was associated with a significant increase in the XMg of growing garnet (Grt2) reflected by garnet chemical zoning (Fig. 6b and d).



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Fig. 9. The PT path (continuous black line) derived for the metamorphic evolution of sample A-258 (locality 1 in Fig. 1). {square}, PT data for the early generation of garnet (Grt1); {blacksquare}, PT data for the later generation (Grt2). (a) PT path and compositional isopleths for the garnet + sillimanite + cordierite + quartz assemblage. (b) Relationship of PT path to isopleths of garnet mode [atomic ratio 100(Mg + Fe)in garnet/(Mg + Fe)in rock]. (c) Calculated equilibrium compositions of minerals along the derived PT path. (d) Calculated equilibrium relative garnet modes along the derived PT path.

 


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Fig. 10. The PT path (continuous black line) derived for the metamorphic evolution of sample A-275 (locality 1 in Fig. 1). {square}, PT data for the early generation of garnet (Grt1); {blacksquare}, PT data for the later generation (Grt2). (a) PT path and compositional isopleths for the garnet + sillimanite + cordierite + quartz assemblage. (b) Relationships of PT path with isopleths of relative garnet mode [atomic ratio 100(Mg + Fe)in garnet/(Mg + Fe)in rock]. (c) Calculated equilibrium compositions of minerals along the derived PT path. (d) Calculated equilibrium relative garnet modes along the derived PT path.

 


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Fig. 11. The PT path (continuous black line) derived for the metamorphic evolution of sample A-538 (locality 2 in Fig. 1). {square}, PT data for the early generation of garnet (Grt1); {blacksquare}, PT data for the later generation (Grt2). (a) PT path and compositional isopleths for the garnet + sillimanite + cordierite + quartz assemblage. (b) Relationships of PT path with isopleths of relative garnet mode [atomic ratio 100(Mg + Fe)in garnet/(Mg + Fe)]in rock]. (c) Calculated equilibrium compositions of minerals along the derived PT path. (d) Calculated equilibrium relative garnet modes along the derived PT path.

 


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Fig. 12. The PT path (continuous black line) derived for the metamorphic evolution of sample A-643 (locality 2 in Fig. 1). {square}, PT data for the early generation of garnet (Grt1); {blacksquare}, PT data for the later generation (Grt2). (a) PT path and compositional isopleths for the garnet + sillimanite + cordierite + quartz assemblage. (b) Relationships of PT path with isopleths of relative garnet mode [atomic ratio 100(Mg + Fe)in garnet/(Mg + Fe)in rock]. (c) Calculated equilibrium compositions of minerals along the derived PT path. (d) Calculated equilibrium relative garnet modes along the derived PT path.

 
We consider the calculated PT coordinates to be sufficiently accurate and these paths to be real. The authenticity of the PT paths is supported by: (1) consistency of the calculated PT trajectories with both reaction textures and mineral zoning (Figs 912); (2) negligible influence of late diffusion (e.g. Frost & Chacko, 1989Go; Spear & Florence, 1992Go) on the strong increase in XMg of garnet toward the contacts with cordierite (Fig. 6b and d). Furthermore, the use of the same geothermobarometric equations for all studied samples suggests that a valid comparison between the PT paths obtained, which is essential for our study, depends on the accuracy of analytical data only. Uncertainties in the thermodynamic data that propagate into uncertainties in the general position and orientation of the PT paths have no major effect on such a relative comparison.

Table 4 contains the compositions of garnet and biotite coexisting with K-feldspar, sillimanite and quartz in the studied samples. Using these compositions, water activity along the PT paths was also estimated (Table 4). All studied samples are characterized by a low water activity (0·15–0·30) that generally decreases with falling temperature. The systematic lowering of water activity after peak metamorphic conditions is consistent with the dehydration reaction textures observed in the metapelites (e.g. Fig. 4c).


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Table 4: Selected P–T–aH2O parameters of garnet–biotite–sillimanite–K-feldspar–quartz equilibria for samples from Table 1

 

    NUMERICAL MODELLING OF PT PATHS
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
The metapelites of the Kanskiy granulite complex exhibit characteristic garnet-forming reaction textures and flat PT cooling paths that are consistent with previously published data on this complex (Perchuk et al., 1989Go). However, an important new result from this study is the distinct difference in the shape of PT paths from different parts of the Kanskiy granulite complex: (1) metapelites collected far (~8 km) from the boundary with the lower-grade Yeniseyskiy complex (e.g. A-538, A-643, Fig. 1) followed a simple, essentially linear near-isobaric cooling path with dP/dT = 0·005–0·006 kbar/°C; (2) metapelites collected close (~3 km) to this boundary (e.g. A-258, A-275, Fig. 1) reveal a kinked PT path with an intermediate interval of burial cooling (dP/dT = –0·005 to –0·006 kbar/°C). The difference in the shape of the PT paths is supported by reversals in garnet zoning in the second group of samples (e.g. A-275, Fig. 7b).

The diversity of PT paths in the granulites from the Kanskiy granulite complex (Fig. 13) is not unique. As indicated in Fig. 2, similar features have been found in other high-grade terrains such as the Limpopo granulite complex in South Africa (Perchuk et al., 1996Go, 2000bGo; Smit et al., 2001Go), the Lapland complex in the Kola Peninsula (Perchuk et al., 1999Go, 2000bGo), and the Sharizhalgay complex in the Baikal area, Eastern Siberia (Perchuk, 1989Go). This underscores the general importance of the phenomenon and suggests a systematic genetic pattern indicative of a specific geodynamic process.



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Fig. 13. Summary of PT paths for metapelites of the Kuzeevskiy (Perchuk et al., 1989Go) and Atamanovskiy (this study) sequences of the Kanskiy granulite complex.

 
The existence of kinked PT paths for metapelites of the Limpopo high-grade terrain (Fig. 2) was first described by Perchuk et al. (1996Go, 2000b)Go, who noted that kinked PT paths with low dP/dT cooling portions are characteristic of samples collected close (<45 km) to the boundary of the complex with the Kaapvaal Craton. Perchuk et al. (1996Go, 2000bGo) explained the existence of these two types of PT paths by differences in the relative movement of different crustal blocks during their exhumation. The crustal blocks from central portions of the granulite complex were subjected to straightforward exhumation, allowing their adjustment to the ambient thermal gradient. On the other hand, the PT evolution of ascending blocks close to the boundary of the complex was disturbed at crustal levels of about 13–15 km, where rapid cooling was initiated because of the temperature gradient between the hot granulites and the cooler overridden cratonic rocks.

A physical test of these ideas has been provided by numerical geodynamic experiments (Gerya et al., 2000Go) based on the gravitational redistribution mechanism suggested by Perchuk (1989)Go and Perchuk et al. (1992)Go for the exhumation of granulites. Taking into account the inherent gravitational instability (Gerya et al., 2001Go, 2002Go) of hot continental crust subjected to the regional low- to medium-pressure granulite-facies conditions characteristic for the Kanskiy complex (Fig. 13), the presence of large amounts of low-density, syn- to late-tectonic granitic rocks within the complex, and thrusting of the granulites of the Kanskiy complex over the lower-grade rocks of the Yeniseyskiy and Yukseevskiy complexes (Smit et al., 2000Go), the gravitational redistribution (diapiric) model could also be applicable to the studied region.

Figure 14 presents the results of numerical modelling of the buoyant exhumation of a granulite complex scaled to represent the Kanskiy complex from middle crustal depths along the weak tectonic zone formed at a boundary between two cratons (Gerya et al., 2000Go). This model suggests thrusting of hotter and less dense granulite onto the colder and more dense middle- and upper-crustal complexes. High (102) viscosity contrast between weaker granulites and stronger lower-grade rocks results in the intensely complicated internal deformation of the granulite complex associated with the moderate localized planar deformation of the lower-grade complexes.



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Fig. 14. Results of numerical modelling (Gerya et al., 2000Go) of the buoyant exhumation of a granulite complex. Model design: size 100 km x 30 km; grid resolution 100 x 30 nodes, 500 x 150 markers; rock types are sediments (white, {rho} = 2700 kg/m3, {eta} = 1019 Pa s, where {rho} is density and {eta} is viscosity), felsic granulites (light grey, {rho} = 2800 kg/m3, {eta} = 1019 Pa s), metabasites (dark grey, {rho} = 3000 kg/m3, h = 1019 Pa s at T > 600°C in granulite sequence, {eta} = 1021 Pa s at T < 600°C in greenstone sequence), metakomatiites (black, {rho} = 3300 kg/m3, {eta} = 1021 Pa s) and weak tectonic zone (dashed, {eta} = 1019 Pa s for all rock types); heat conductivity of rocks is 4 W/m per K; isobaric heat capacity of rocks is 1100 J/kg per K. Initial conditions: {partial}T/{partial}x = 0, {partial}T/{partial}z = 0·03 K/m, where x and z are horizontal and vertical coordinates, respectively. Boundary conditions: top—free slip, T = 27°C; bottom—no slip, T = 927°C; walls—no slip, {partial}T/{partial}x = 0.

 
An important observation consistent with the petrological data presented here concerns the calculated PT trajectories (Fig. 15) of rock fragments within the exhuming granulite complex (see the two markers in Fig. 14): (1) the fragment exhumed close to the boundary of the complex is characterized by a kinked PT path (see square marker in Figs 14 and 15), whereas (2) the fragment exhumed far from this boundary shows a linear PT trajectory (see round marker in Figs 14 and 15). The numerical modelling suggests (Figs 14 and 15) that the isobaric cooling or even burial cooling intervals of kinked PT paths reflect interaction between an exhuming hot granulite body on the one hand and an overridden cooler cratonic plate on the other. This interaction results in a local convective cell, which causes sub-horizontal movement of granulite towards the cool plate (Fig. 14). This process is typical for the early diapiric uprising stages (0–2 Myr) characterized by significant transient disturbance of the thermal field owing to the rapid (5–10 mm/yr) movement of rocks from different crustal levels (Fig. 14). At the later diapir expansion stages (2–10 Myr), this disturbance vanishes as a result of the decrease in material displacement rates (1–5 mm/yr). Consequently, the rocks exhumed at this latter stage followed simple linear PT trajectories (see round marker in Figs 14 and 15).



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Fig. 15. The results of numerical modelling of PT–time paths for two granulitic fragments shown in Fig. 14. Pressure along the PT paths is calculated as a function of depth neglecting nonlithostatic (e.g. Manktelov, 1995Go; Petrini & Podladchikov, 2000Go) component.

 
This modelled scenario of buoyant exhumation of a granulite complex is also consistent with the results of a recent structural–metamorphic study of the Southern Yenisey Range by Smit et al. (2000)Go, which confirms thrusting of the relatively hot and ductile granulites of the Kanskiy complex onto the relatively cold and stiff lower-grade rocks of the Yeniseyskiy and Yukseevskiy complexes. The gravitational redistribution model also predicts the selective accumulation of basic granulites at the tectonic boundary with the overridden lower-grade rocks. This process is related to the differential movement of high-density basic and lower-density felsic rock units within exhuming granulite body (Fig. 14). This prediction is supported by an increase in the relative amount of metabasites within the Kanskiy complex toward the NW contact with the Yeniseyskiy complex (Nozkhin & Turkina, 1993Go).


    CONCLUSION
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
The PT paths derived in this paper for the Kanskiy complex of Eastern Siberia on the basis of thermobarometry and analysis of reaction textures provide another example of contrasting dP/dT development in a granulite complex as a function of distance to the enclosing lower-grade rock sequences. The shapes of the PT paths found are in accordance with ideas on buoyant exhumation mechanisms for granulites as suggested by Perchuk (1989)Go and Perchuk et al. (1992)Go, as well as numerical and analytical models of Gerya et al. (2000Go, 2001Go, 2002Go) for such a process. In a more general sense, we show that such a diversity of PT paths for a given geodynamic scenario is a logical consequence of the different possible physical trajectories of rocks in a variable thermal field (both in space and time) disturbed by rapid differential movement of material from different crustal levels. Any major geodynamic (i.e. orogenic) process may lead to an array of diverse but interrelated PT paths recorded by metamorphic rocks (e.g. Willner et al., 2002Go) from different localities within the complex. Conversely, the nature of this array will provide definitive evidence for the nature of the geodynamic process itself.


    SUPPLEMENTARY DATA
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
Supplementary data for this paper are available at Journal of Petrology online.


    ACKNOWLEDGEMENTS
 
The authors appreciate the help of E. V. Guseva and N. N. Korotaeva during the microprobe study. This work was carried out through the support of RFBR grant 03-05-64633, an Alexander von Humboldt Foundation Research Fellowship to T.V.G. and the Sonderforschungsbereich 526 at Ruhr-University Bochum, funded by the Deutsche Forschungsgemeinschaft. Constructive reviews by Michael Brown and Chris Carson are greatly appreciated.


    FOOTNOTES
 

* Corresponding author. Present address: Institut für Geologie, Mineralogie und Geophysik, Ruhr-Universität Bochum, Universitätstrasse 150, 44780 Bochum, Germany. Telephone: 49-234-3223518. Fax: 49-234-3214433. E-mail: taras.gerya{at}ruhr-uni-bochum.de


    REFERENCES
 TOP
 ABSTRACT
 INTRODUCTION
 GEOLOGICAL SETTING
 GEOLOGY OF THE KANSKIY...
 MINERALOGY AND PETROLOGY OF...
 THERMOBAROMETRY AND P-T PATHS
 NUMERICAL MODELLING OF P-T...
 CONCLUSION
 SUPPLEMENTARY DATA
 REFERENCES
 
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