14–15 Nov 2024
熊取交流センター すまいるズ 煉瓦館
Asia/Tokyo timezone

Measurement of neutron capture cross-sections of $^{99}$Tc at ANNRI of J-PARC MLF/J-PARC MLF ANNRIを用いた$^{99}$Tcの中性子捕獲断面積の測定

14 Nov 2024, 16:00
2h
熊取交流センター すまいるズ 煉瓦館

熊取交流センター すまいるズ 煉瓦館

大阪府泉南郡熊取町五門西1丁目10番1号

Speaker

Maloney/マロニー Maxwell Clark/マックスウェルクラーク (Institute of Science Tokyo/東京科学大学)

Description

Technetium-99 is a long-lived fission product (LLFP) which undergoes $\gamma$-decay with a half-life of 211,100 years. This long-lived nature and relative abundance of production (approximately 6% of fission events produce $^{99}$Tc) and environmental mobility makes long term waste storage challeng-ing. As such it is a possible candidate for being reduced via nuclear transmutation. The $^{99}$Tc(n, γ)$^{100}$Tc produces $^{100}$Tc which undergoes $\gamma$-decay to the stable $^{100}$Ru with a half-life of 15.46 min. To design systems that could drive these reactions, more accurate neutron capture cross-section data is required. There are large differences between experimental data of the neutron capture cross-sections, especially in the keV neutron energy range [1][2][3][4]. This motivated the present measurement of the neutron capture cross-sections of $^{99}$Tc.

The experiment was conducted at the Accurate Neutron-Nucleus Reaction measurement In-strument (ANNRI) beamline at the Materials and Life Science Experimental Facility (MLF) at the Japan Proton Accelerator Research Complex (J-PARC). Capture $\gamma$-rays from neutron capture events were measured using a NaI(Tl) detector placed at a 90 degree angle to the neutron beam axis. The total mass of the 99Tc sample was 78 mg with a diameter of 6.3 mm and an activity of 1.4 mCi at time of preparation and was contained in an aluminum sample case. The sample was placed at a neutron flight distance of 27.9 m and capture $\gamma$-rays were measured from thermal to the keV energy range. The time-of-flight (TOF) method was employed to determine the incident neutron energy. The incident neutron spectrum was determined by placing a sample of boron enriched with 10B at the sample position and detecting 478-keV γ-rays from the $^{10}$B(n,γ)$^{7}$Li reaction. A blank run, a dummy case and a carbon sam-ple were also measured for the purposes of background subtraction. From this raw TOF spectrum the neutron capture yield was calculated using the pulse height weighting technique. Self-shielding and multiple scattering were accounted for using PHITS simulation code. The neutron capture-cross section of $^{99}$Tc from the thermal to keV energy region were derived. This presentation will compare present results with past data and provide a discussion.

References:
[1] G. Noguere et al. Phys. Rev. C, 102, 015807 (2020).
[2] N. Iwamoto Journal of Nuc. Sci. and Tech., Vol. 49, No. 2 (2012).
[3] D. Rochman et al. Nuc. Sci. and Eng., 158, 68-77 (2008).
[4] N. Iwamoto et al. EPJ Web of Conferences, 146, 02049 (2017).

Primary author

Maloney/マロニー Maxwell Clark/マックスウェルクラーク (Institute of Science Tokyo/東京科学大学)

Co-authors

Atsushi/敦 Kimura/木村 (JAEA/日本原子力研究開発機構) Chikako/知香子 Ishizuka/石塚 (Institute of Science Tokyo/東京科学大学) Gengchen/庚辰 Li/李 (Institute of Science Tokyo/東京科学大学) Gerard Rovira (JAEA/日本原子力研究開発機構) Hiromi/大洋 Kondo/近藤 (Institute of Science Tokyo/東京科学大学) Jiamo/佳黙 Han/韓 (Institute of Science Tokyo/東京科学大学) Shoji/詔司 Nakamura/中村 (JAEA/日本原子力研究開発機構) Shunsuke/駿典 Endo/遠藤 (JAEA/日本原子力研究開発機構) Tatsuya/竜也 Katabuchi/片渕 (Institute of Science Tokyo/東京科学大学) Zefeng Shao (Institute of Science Tokyo/東京科学大学)

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