Apatite fission tracks are immediately annealed at temperatures
110C (e.g., Wagner and Van den Haute, 1992). At
temperatures less than about 60C, apatite fission tracks are
completely preserved. The temperature zone between 60 and
110C is named the apatite fission track partial
annealing zone (e.g., Dumitru, 2000). In this zone, fission tracks
are not immediately annealed, but gradually shortened with time. The
annealing temperature of zircon fission tracks is more controversial,
but generally considered to lie between 230 and 310C (see
discussion by Tagami and Dumitru, 1996). In this paper, we will assume
the more ``conservative'' value of 230C.
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First, we will discuss the apatite fission track data (Figure
2). Of the five Great Valley Group samples, four have
exclusively Cretaceous apatite fission track grain-ages, indicating
that these grains never reached temperatures greater than 110C
since their deposition in the Great Valley Group. However, sample JR2
has the oldest depositional age of these four samples but the youngest
fission track ages, with the latter being even slightly younger than
the former. Therefore, JR2 has been partially reset, and saw
temperatures less than 110C, but well above 60C.
The fission tracks of sample JR2 are also significantly shorter than
those of the other samples, an additional suggestion that JR2 must
have been heated to well within the partial annealing zone. Sample
JR1, located the nearest to the New Idria serpentite, has completely
annealed apatite fission tracks and, therefore, was heated above
110C. It dates the end of the heating event at 14
Ma. Sample JR6 from the Miocene Temblor Formation contains two age
components: one Cretaceous and one Miocene component (Table
2). There also is a hint of bimodality in the fission
track length distribution. A first group of relatively short
(9-13 m) fission tracks formed prior to the mid-Miocene.
These tracks preserve Sierran provenance ages but were partially
annealed during the mid-Miocene thermal event. A second group of long
fission tracks (13-17 m) formed after this thermal event,
and have not been annealed since then. Paleocurrent directions in the
Temblor and Big Blue Formations are west-to-east, which is the
opposite flow direction as for the Great Valley Group (Casey and
Dickinson, 1976; Bate, 1985; Bent, 1985). Therefore, the apatite
grains of the Temblor Formation have been redeposited from the
underlying Great Valley Group, some of which was thermally annealed
during a mid-Miocene thermal event.
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The zircon fission track ages for four of the five samples are older than the age of Great Valley Group deposition (Figure 3). Sample JR1, which had completely annealed apatite fission tracks, also has unreset zircon fission track ages. Therefore, sample JR1 was heated to more than 110C, but less than 230C after its deposition. The lag between crystallization, exhumation and deposition times were short, which means that the source area of these sediments exhumed rapidly. The most surprising observation is that the Middle Miocene sample JR6, which had a bimodal apatite fission track age distribution, also has a bimodal zircon fission track distribution. The oldest mode of Mesozoic ages is compatible with the unreset fission track ages of the Joaquin Ridge samples located away from the serpentinite body (Table 1). The youngest age peak is concordant with the 14 Ma apatite fission track age of sample JR1, and with the youngest mode of the apatite fission track age distribution of JR6. Because not all the apatite grains in JR6 were reset at 14 Ma, we know that this sample was not heated to more than 110C. In fact, there is ample evidence that the Temblor formation did not see temperatures higher than 56C east of Joaquin Ridge (see below). Therefore, the 14 Ma old zircons must have been been annealed prior to deposition in the Temblor and Big Blue formations. Recalling the eastward paleocurrents of these deposits, this indicates that at least part of the provenance area for the Temblor Formation, which is Joaquin Ridge, reached temperatures as high as 230C as recently as 14 Ma.