HR: 1340h
AN: V13A-0512 [Abstracts]
TI: (U-Th)/Ne Chronometry
AU: * Gautheron, C E
EM: gautheron@geol.u-psud.fr
AF: Division of Geological and Planetary Sciences, MS100-23, California Institute of Technology, Pasadena,
CA CA91125
United States
AU: Tassan-Got, L
EM: tassango@ipno.in2p3.fr
AF: Institut Physique Nucléaire, Bat 102, Université Paris XI, Orsay,
91405
France
AU: Farley, K A
EM: farley@gps.caltech.edu
AF: Division of Geological and Planetary Sciences, MS100-23, California Institute of Technology, Pasadena,
CA CA91125
United States
AB:
Nuclear production of 21Ne, like 4He, in U and Th rich minerals such as apatite, zircon, monazite and titanite can
potentially be used for chronometry. Due to the absence of 24Mg from the accessory minerals of interest, the production
of 21Ne through neutron-induced reactions can be neglected and this production only occurs through the reaction
18O(α,n)21Ne. As the closure temperature is higher for neon than for helium, this gives a possible insight
to the thermal history of minerals. To test the possibility of this new chronometer, a review of the available cross section
data has been done, permitting a reevaluation of the 21Ne production from this reaction, using a thin target approach
and testing the validity of the results against thick target situations. The important factors of the simulation are the
cross section and the stopping distance values for a mineral characterized by its chemical composition and density. The
(21Ne/4He) production ratio in these minerals is about 4× 10-8, but varies with oxygen content and Th/U
ratio. Although the 21Ne has a stopping range of about 1 μm compared to about 20 μm for α particles,
preferential α ejection compared to 21Ne lowers (21Ne/4He) at grain edges. For a bulk crystal the
(21Ne/4He) production ratio depends on crystal size when the crystals are small. Using a Monte Carlo model we
computed the effects of ejection on the (21Ne/4He) ratio for various geometries and grain sizes. The simulation can
be run by any user through a graphical interface accessible from the Web at the address:
http://h0.web.u-psud.fr/UThHeNe_MonteCarloSimulation/.
We also present measurements of the (21Ne/4He) ratio on few mg aliquots of well-dated volcanic apatites and
zircons. Values of (4.43± 1.1)× 10-8 and (3.46± 1.2)× 10-8 for apatite and zircon respectively are in
agreement with the theoretical values of (4.16± 0.14)× 10-8; (3.54± 0.13)× 10-8. Based on our
production rate estimates the Durango apatite and Fish Canyon Tuff zircon give Ne ages of 34.2± 8.6 Ma and 28.0± 12.2
Ma respectively, which are in agreement with independently known ages. Our results demonstrate that (U-Th)/Ne can be used as
a chronometer in volcanic samples. Additionally, the 4He and 21Ne content of zircons from the deeply exhumed
crustal section in Gold Butte, Nevada (crystallization age of 1.4 Ga) imply (U-Th)/Ne ages of 963± 164 and 777± 122
Ma, far older than their He ages of 16.7± 1.3 and 19.1± 1.5 Ma respectively. To explain the age difference, a neon
closure temperature for zircon around 400°C is derived.
DE: 1115 Radioisotope geochronology
DE: 1140 Thermochronology
DE: 1744 Tectonophysics
DE: 1749 Volcanology, geochemistry, and petrology
SC: Volcanology, Geochemistry, Petrology [V]
MN: Fall Meeting 2005