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4.4  ·  Lattice-Preferred Orientation (LPO)  109
                 4.4.5                                         olivine is at the limit of crystalplastic behaviour, diffuse
                 LPO Patterns of Other Minerals                girdles of principal axes may occur. At medium tempera-
                                                               ture (≈1000 °C), a girdle of [0kl] normal to L  and a point
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                 As in quartz, LPO in other minerals strongly depends on  maximum of [100] parallel to L  may form. At high tem-
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                 active slip systems and on the geometry and symmetry  perature (>1100 °C) a point maximum of [010] normal
                 of the flow pattern, resulting in a similarity of LPO geom-  to S  and [100] parallel to L  develops; and at hypersolidus
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                 etry and strain geometry. As for quartz, slip systems and  conditions (>1250 °C) a point maximum of [100] paral-
                 fabric elements tend to rotate towards the fabric attractor,  lel to L  and partial girdles of [010] and [001] are formed.
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                 resulting in a common subparallel orientation of compo-  Fabrics with external asymmetry do occur and can be
                 nents of the LPO, and S  and L  in the rock.  used to determine shear sense (Avé Lallemant and Carter
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                   Calcite c-axis LPO patterns show a similar influence  1970; Mercier 1985).
                 of flow symmetry on pattern geometry. At low tempera-  In clinopyroxene three main types of LPO have been
                 ture (<300 °C) coaxial progressive flattening produces a  described; (a) [100] normal to S  and [001] parallel to L  or
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                 maximum around the Z-axis of strain. In constriction a  S  (Mainprice and Nicolas 1989; Phillipot and van Roermund
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                 girdle through Y and Z develops and in coaxial plane  1992); (b) [010] normal to S  and [001] parallel to L  or S r
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                 strain a maximum around Z and a minor girdle through Y  (Mainprice and Nicolas 1989); (c) [010] normal to L  and
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                 (Wenk et al. 1986a; Shelley 1993). In simple shear flow, a  [001] parallel to L  (Helmstead et al. 1972; van Roermund
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                 c-axis girdle develops as for quartz, but dipping in the  1983, 1992). (a) is mainly found in peridotite massifs with
                 opposite direction (in the direction of the shortening ISA).  pyroxenite layers and may either be formed at low tempera-
                 This is due to the fact that in calcite at low temperature, e-  ture and high strain rate or, if this is unlikely, by post-tec-
                 twinning is largely responsible for development of the LPO  tonic crystal growth (van Roermund 1992). (b) and (c) form
                 fabric (Schmid 1982; Behrmann 1983; Schmid et al. 1987;  by crystalplastic deformation by multiple slip in medium
                 Wenk et al. 1987; Rutter et al. 1994; Lafrance et al. 1994;  to high temperature eclogites by activity of dislocations
                 Rutter 1995; Khazanehdari et al. 1998; Casey et al. 1998;  with predominantly [001] and <110> Burgers vectors (van
                 Pieri et al. 2001).                           Roermund 1983, 1992; Buatier et al. 1991). Their difference
                   Experimental and computer models indicate that at  seems to reflect different strain types, constriction for
                 high temperature in plane strain, split maxima may de-  Type (b) and flattening for Type (c) (Helmstead et al. 1972;
                 velop around the shortening axis (Wagner et al. 1982;  van Roermund 1992). Asymmetric fabrics have not been
                 Wenk et al. 1986a, 1987; Schmid et al. 1987; Takeshita et al.  reported for clinopyroxene in the literature.
                 1987; de Bresser 1991). Natural examples of such a high  In orthopyroxene deformed at high-grade metamor-
                 temperature LPO pattern in calcite were reported by de  phic conditions, LPO of [100] has been reported at a high
                 Bresser (1989), Burlini et al. (1998), Kurz et al. (2000), Leiss  angle to S  and of [001] gently inclined with respect to L r
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                 and Molli (2003) and Barnhoorn et al. (2004).  (Dornbush et al. 1994). This preferred orientation is as-
                   In plagioclase, (010) trends to parallelism with S  and  sociated with the dominance of (100)[001] as a slip sys-
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                 [001] with L  at medium to high-grade metamorphic con-  tem. The LPO reported by Dornbush et al. (1994) is slightly
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                 ditions (Olsen and Kohlstedt 1985; Montardi and Mainprice  asymmetric and can be used to determine sense of shear.
                 1987; Ji and Mainprice 1988; Shaosheng and Mainprice 1988;  Little is known about LPO in amphiboles, but the avail-
                 Mainprice and Nicolas 1989; Dornbush et al. 1994; Egydio-  able data indicate a strong similarity with clinopyroxene.
                 Silva and Mainprice 1999). At very high grade, however,  [001] is commonly parallel to L  (Gapais and Brun 1981;
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                 [100] trends to parallelism with L  (Kruhl 1987b; Dorn-  Rousell 1981; Shelley 1994) and either (100) (Mainprice
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                 bush et al. 1994). In shear zones, the pole to (010) tends to  and Nicolas 1989) or (110) (Gapais and Brun 1981) paral-
                 show an external asymmetry with respect to a planar and  lel to S . Preferred orientations at medium to high grade
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                 linear shape preferred orientation, which can be used to  may be due to crystalplastic deformation, but LPO in
                 determine shear sense as in the case of quartz c-axes.  amphiboles at low-grade conditions may be due to rigid
                   Olivine has a complex behaviour that is strongly de-  body rotation, dissolution-precipitation or oriented
                 pendent on temperature (Mainprice and Nicolas 1989).  growth (Ildefonse et al. 1990; Shelley 1993, 1994; Imon et al.
                 At relatively ‘low’ temperatures (700–1 000 °C) corre-  2004). Hornblende fabrics reflect the strain symmetry
                 sponding to lower crustal or upper mantle levels where  (Gapais and Brun 1981).
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