EGU25-15502, updated on 15 Mar 2025
https://doi.org/10.5194/egusphere-egu25-15502
EGU General Assembly 2025
© Author(s) 2025. This work is distributed under
the Creative Commons Attribution 4.0 License.
Poster | Tuesday, 29 Apr, 10:45–12:30 (CEST), Display time Tuesday, 29 Apr, 08:30–12:30
 
Hall X2, X2.73
ESR-thermochronometry of the MIZ1 borehole, Tono, Japan
Georgina King1, Lily Bossin1,2, Melanie Kranz-Bartz1,3, Xiaoxia Wen1, Christoph Schmidt1, Frederic Herman1, Manabu Ogata4, and Shigeru Sueoka4
Georgina King et al.
  • 1University of Lausanne, Institute of Earth Surface Dynamics, Lausanne, Switzerland (georgina.king@unil.ch)
  • 2Paul Scherrer Institute, Villigen, Switzerland
  • 3Institute of Geology, Mineralogy, and Geophysics, Ruhr-University Bochum, Germany
  • 4Tono Geoscience Center, Japan Atomic Energy Agency, Toki, Japan

Electron spin resonance (ESR) dating of quartz minerals offers a significant advantage over luminescence dating because of its later signal saturation. We seek to exploit this to develop a thermochronometry system capable of resolving rock cooling rates throughout the Quaternary. Whereas the luminescence thermochronometry system is limited to areas experiencing very rapid rock cooling (exhumation) of tens of mm/yr, recent studies have shown that ESR thermochronometry can resolve rates of <1 mm/yr over Quaternary timescales (e.g. Bartz et al., 2024). However, the method has not yet been validated against samples with known thermal histories. To this end, we have investigated six known-thermal history samples from the MIZ1 borehole, Tono, Japan. The low-relief Tono region, Japan, underwent Quaternary exhumation at rates of <1 mm/yrand previous luminescence thermochronometry (Ogata et al., 2022) on the same samples yielded saturated signals. Sample borehole temperatures range from 22.7 to 43.8 °C.

The natural trapped-charge concentration of the different samples was constrained using a single-aliquot regenerative dose measurement protocol. As the samples had similar properties, we constructed a standardised growth curve to alleviate measurement times. Signal saturation of the Al-centre occurred at ~60 kGy and at ~7 kGy for the Ti-centre. Whereas the Al-centre exhibited single-saturating exponential growth, the Ti-centre exhibited significant sub-linearity in the low dose region, within which the natural trapped-charge concentrations were interpolated.

The thermal stability of the different samples was measured using an isothermal holding experiment, whereby samples were dosed in the laboratory before being held at fixed temperatures (130 °C, 160 °C, 200 °C, 250 °C), for durations ranging from 4 min up to a cumulative duration of 10 h. As the thermal signal loss of the different samples was similar, we were able to fit all samples to derive a single set of thermal kinetic parameters.

Finally, the data were inverted for borehole temperature using a Monte-Carlo approach. Whereas the Al-centre of all samples recovered borehole temperature within 1s uncertainties, the Ti-centre data failed to recover temperature, yielding temperatures ~20-30 °C above borehole temperature. The cause for this is uncertain but is likely related to the observed sub-linearity of the dose response curves which may be indicative of sensitivity change throughout analysis.

 

 

Bartz, M., King, G.E., Bernard, M., Herman, F., Wen, X., Sueoka, S., Tsukamoto, S., Braun, J. and Tagami, T., 2024. The impact of climate on relief in the northern Japanese Alps within the past 1 Myr–The case of the Tateyama mountains. Earth and Planetary Science Letters644, p.118830.

Ogata, M., King, G.E., Herman, F. and Sueoka, S., 2022. Reconstructing the thermal structure of shallow crust in the Tono region using multi-OSL-thermometry of K-feldspar from deep borehole core. Earth and Planetary Science Letters591, p.117607.

How to cite: King, G., Bossin, L., Kranz-Bartz, M., Wen, X., Schmidt, C., Herman, F., Ogata, M., and Sueoka, S.: ESR-thermochronometry of the MIZ1 borehole, Tono, Japan, EGU General Assembly 2025, Vienna, Austria, 27 Apr–2 May 2025, EGU25-15502, https://doi.org/10.5194/egusphere-egu25-15502, 2025.