Measurement of the natDy(p,x) nuclear reactions cross-sections

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Abstract

Excitation functions of the reactions natDy(p,x)159m+gHo, 161m+gHo, 162mHo, 162gHo, 155m+gDy, 157m+gDy, 159m+gDy, 155Tbcum, 155Tb, 156Tbcum, 160Tb, 161Tb, 159m+gGd were measured in the energy range of 7.4–35.9 MeV using the stacked foil technique and off-line γ-ray spectrometry. The obtained cross-sections were compared with previously published experimental data and prediction of the TALYS nuclear reaction model code adopted from the TENDL-2019 library. Thick target yields were calculated from the experimental data.

Introduction

Radionuclide 161Tb (T½ = 6.89 d) is a promising alternative to the established therapeutic 177Lu. It emits low energy β particles with mean energy of 154 keV and maximum energy of 593 keV. Moreover, it provides more conversion and Auger electrons that may enhance its therapeutic efficacy compared to 177Lu [1], [2].

Terbium-161 is usually produced in nuclear reactors via neutron capture on highly enriched 160Gd targets, followed by a β decay of the short-lived 161Gd (T½ = 3.66 min) [2]. While the production in nuclear reactors is already well established, its potential production by charged-particle accelerators still deserves our attention. In principle, there are two possible reactions resulting in formation of 161Tb – 160Gd(d,n) and 164Dy(p,α). Excitation function of the latter has been measured only once on natural dysprosium target by Tárkányi et al. and results were published in 2013 [3]. It motivated us to re-measure in detail cross-sections of proton-induced reactions on natDy for all the radionuclides that we could quantify in the activated targets. Cross-sections for the formation of 162gHo and 159m+gGd are published for the first time.

Section snippets

Target and irradiation

Measurement of excitation functions was performed using the standard stacked foil technique. Two stacks of natDy target foils interleaved with titanium monitors and copper degraders were irradiated on the external proton beam of the cyclotron U-120 M at the Nuclear Physics Institute of the Czech Academy of Sciences. The stacks consisted of twelve/thirteen natDy foils (99.9 %, 25 μm thick, Goodfellow, GB), thirteen/fourteen natTi foils (99.6 %, 11.0 μm thick, Alfa Aesar, USA) and optimal

Beam energy and current

Entrance proton beam energies based on the beam orbit position measurement were equal to 36.15 ± 0.20 MeV and 20.04 ± 0.20 MeV for the 1st and 2nd stack of foils, respectively. The beam currents recorded by the beam integrator were 0.734 μA and 0.769 μA for the 1st and 2nd stack of foils, respectively. The entrance beam energies were slightly corrected within their uncertainties to 36.00 MeV and 20.15 MeV using reconstructed natTi(p,x)48V monitoring reaction excitation function in comparison

Conclusion

Excitation functions of reactions natDy(p,x)159m+gHo, 161m+gHo, 162mHo, 162gHo, 155m+gDy, 157m+gDy, 159m+gDy, 155Tbcum, 155Tb, 156Tbcum, 160Tb, 161Tb, 159m+gGd have been measured in the energy range of 7.4–35.9 MeV. Cross-sections of reactions natDy(p,x) resulting in 162gHo and 159m+gGd are reported for the first time. Our data were compared with previously published experimental data and with theoretical prediction of the TALYS code adopted from TENDL-2019 library.

Analysing the excitation

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgements

The authors are grateful to the crew of the U-120 M cyclotron for the irradiations and to Dr. Jan Kameník for kind help with γ-ray spectra measurement on the planar HPGe detector. The work was supported by the Czech Technical Agency (project no. TJ0400138) and by the CANAM infrastructure of the NPI CAS.

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