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          Davies and Halliday (1998) found differences in crystallisation times between
          and within minerals of o10 ky (within error of most individual glass-mineral
          isochrons). Differences of 20–70 ky (up to ca. 300 ky) between feldspar centres
          and rims were also found. They calculated crystal growth rates between 7   10  13
                            1
          and 9   10  14  cm s .
            More recent data of Simon and Reid (2005) show that ages of zircons rims
          overlap with eruption, but centres are up to 150 ky older. The oldest zircon ages are
          significantly younger than those previously obtained by whole-rock-glass-minerals
          Rb–Sr isochrons (Figure 8), and thus reduce the residence times of the Glass
          Mountain magmas to a maximum of 190 ky (Table 6 and Figure 8). The difference
          between the Rb–Sr and U–Pb ages could reflect that the minerals defining the
          Rb–Sr isochrons crystallised earlier than the zircons. However, recent interpreta-
          tions (e.g., Simon and Reid, 2005) propose that the Rb–Sr model isochrons are
          not dating the crystal fractionation. They probably are the result of a complex
                                                   87
          history involving open system, including in situ Rb decay in the reservoir and the
          presence xenocrysts.


          3.4.2. Caldera magma: Bishop Tuff petrological attributes and time scale
          information
          The Bishop magma was thermally (ca. 720–7901C) and compositionally zoned in
                                           87  86
          major and trace elements and also in  Sr/ Sr values (Hildreth, 1979; Christensen
          and DePaolo, 1993; Hildreth and Wilson, 2007) prior to eruption. The first erupted
          units are crystal poor, colder and more evolved than the later ones (Hildreth, 1979).
          Water contents vary from ca. 6 to 4 wt% (Anderson et al., 1989), and a pressure of ca.
          200 MPa was determined for the roof of the reservoir (Wallace et al., 1999). The
          liquidus temperatures of the early and late magmas calculated with MELTS (Ghiorso
          and Sack, 1995) are ca. 795 and 8551C, respectively. The origin of the zoning of the
          Bishop magma has been highly debated and investigated. Hildreth (1979) proposed
          that it resulted from convective circulation driven by thermogravitational diffusion,
          complexation and wall-rock exchange. Other interpretations include crystal liquid
          fractionation (Michael, 1983), side-wall crystallization (Wolff et al., 1990; Bindeman
          and Valley, 2002), wall-rock assimilation (Duffield et al., 1995) or mafic intrusion at
          the base of the reservoir (Hervig and Dunbar, 1992). Hildreth and Wilson (2007)
          have recently proposed that the zoning was created by numerous batches of crystal-
          poor melt released from a mush zone at the floor of the accumulating rhyolitic
          magma body. Crystal-melt fractionation was the dominant zoning process. A major
          role for a magma intrusion at the base of the reservoir for triggering the eruption of
          the Bishop Tuff has been recently proposed by Wark et al. (2007).

          3.4.2.1. Residence times of the Bishop magma. The study of residence times in
          the Bishop magma also started with a long estimate from Christensen and DePaolo
          (1993) who proposed a model of the Bishop magma being mainly liquid for
          long periods of time (e.g., 0.5 My) based on Rb–Sr isotope systematics. A later
          40   39
            Ar/ Ar study by Van den Bogaard and Schirnick (1995) reported ages of glass
          inclusions in quartz at 1.9–2.3 Ma, and thus residence times W1 My. A later
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