FT-α dating: a convenient radiometric dating method for geological glasses using natural fission-track measurement and alpha-ray spectrometry with CR-39.

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Presentation transcript:

FT-α dating: a convenient radiometric dating method for geological glasses using natural fission-track measurement and alpha-ray spectrometry with CR-39 nuclear track detectors Tatsuo Suzuki Faculty of Education, Kagoshima University

Purpose of this study How to measure fission-track ages without the use of reactor neutron irradiation. → combination with α track measurements How to obtain them conveniently with common laboratory equipments. → Is it possible to calculate FT age from U content, etched track length?

FT age calculation ρ s = λf/λ ・ N ( e λT – 1) Eq(1) ρ s : spontaneous fission track density (n/cm 2 ) λf : decay constant of spontaneous fission of U-238 λ : total decay constant of U-238 N : number of atoms of of U-238 T : age (yr) N = Rf /2 ・ d ・ 6.022E+23/ / I2382 ・ C Eq(2) Rf : etched track range (Maximum track length + bulk etched depth of sample surface) (cm) d : density of sample (g/cm 3 ) C : uranium content (g/g) I238 : isotopic abundance of U-238

Uranium content determination Alpha track counting from CR-39 detectors placed on sample surface for several months to several years to exposure for alpha particles. Track size distribution measurements by an image processor. Comparison of track size distribution patterns with pellets of powder samples standard material: IAEA RGU1 and IAEA RGTh1.

Alpha track measurements using CR-39 detectors CR-39: BARYOTRACK (Fukubi Chemical Co., Japan) Etching: 6M KOH solution at 70 ℃ for 90 min. Counting: Optical Microscope with reflected light at magnification of ×1000. Track size measurements: an image processor (Digimo Co., Japan)

Moldavite01 Scale: 10 micrometers

RGU RGTh

1. Loading Original Photograph

2. Digitized

3. Reversing digitized Photograph

4. Filled empty spaces

4. Image analyzing

Size distribution patterns

Fitting of distribution patterns R = (C(i)-AxU(i)-BxTh(i)) 2 Ax= 1/(1 + ThUx) Bx= 1/(1 + 1/ThUx) ThUx = Th/U (activity ratio) Finding minimum value of R with the vorious values of the parameter of Th/U

Alpha track measurements Duration of α t racks Th/U ( * ) Estimeted Reference ExposureNo. tracksTrack density Relative toUThU (days)counted(n/cm2)(n/cm2/day)RGU (μ g / g) RGU E E RGTh E E N E E Mld E E E

Etched track length measurements Making replicas of etched surface using silicon resin. Measurements of etch pit heights of vertical tracks (Vt) to the surface by Laser Scanning Microscope. Measurements of etched depth (Vb) of the surface by comparison with the area covered by wax during the etching with 48% HF for glasses also by Laser Scanning Microscope (VK8500, Keyence Co., Japan) Rf = Vt + Vb

Fission tracks in Moldavite Spontaneous tracks Induced and Spontaneous tracks

Calculation of FT-α age for Moldavite U: 5.54 μg/g Th: 11.1 μg/g Rf = 2.61 μm d ≈ 2 g/cm 3 λ f = 8.45 × /yr T = 13.6 Ma

Conclusions Conventional age determination using spontaneous fission track counting and uranium content estimation from alpha spectrometry based on track size measurements with an image processer and CR-39 nuclear track detectors was tentatively applied to determine the age of Moldavite. Uranium and thorium content of IAEA reference samples usually used for gamma radiation measurements are also useful for alpha track measurements but it would be much better to pulverize them as much more fine state. These experiments can be applied also to other geological glasses although it needs long exposure duration as several years for alpha particles.

References Browne, E., Firestone, R.B. and Shirley, V.S (1986) Table of Radioactive Isotopes. Wiley-Interscience Hadler N., J.C., Iunes, P.J., Osorio A, A.M. and Paulo, S.R. (1991) Relationship between track size and energy for alpha particles in CR-39. Nucl. Tracks Radiat. Meas., 19, 1-4, Hadler N., J.C., Iunes, P.J., Paulo, S.R., Policatro, A.P. and Tello S., C.A. (1995) A discussion on the reliability of alpha-spectroscopy using CR-39 and an image processor. Radiat. Meas., 25, 1-4, Hosoe, M., Takami, Y., Shiraishi, F. and Tomura, T. (1984) Stopping power measurement using thick alpha sources. Nucl. Instr. Methods Phys. Res., 223, Takami, Y., Hashimoto, T., Shiraishi, F. and Voss, K. (1986) Quantitative analysis of alpha activities in thick sources using Si detectors. IEEE Tracsact. Nucl. Sci., 33, 1,

SampleTh ppm U ppmRaTh/UTh/U act. S S S S S S IAEA × IAEA × IAEA × RGU-1< < 2.5× RGTh NBS SRM

2.Samples Samples used in this work are IAEA nuclear reference material of uranium ore: S-13, S-8 and S-7, Thorium ore: S-14, S-15 and S-16, Environmental Materials: IAEA-312, IAEA-313 and IAEA-314, and Gamma-ray Spectrometry Reference Materials: RGU-1 and RGTh-1. The certificated data of Ra, Th and U content by IAEA are summarized in Table. SampleTh ppm U ppmRaTh/U Th/U activity S S S S S S IAEA IAEA IAEA RGU-1< < 2.5× RGTh NBS SRM

Comparison of size distribution patters RGU2RGThS8S14S15N610I312I313i314Mold01 A(C(4)-C(7)) B(C(7)- C(13)) B/A Th/U act (Reference) C(Size)RGU2RGThS8S14S15N610I312I313i314Mold RGU2RGThS8S14S15N610I312I313i314Mold01 A(C(4)-C(7)) B(C(7)-C(13)) B/A Th/U act (Reference) C(Size)RGU2RGThS8S14S15N610I312I313i314Mold

S8 S14

IAEA314 Scale: 10 micrometers

IAEA312 IAEA 313