Production of the 178m2Hf isomer in nuclear reactor

Oct 17, 2020, 2:35 PM
25m
Online

Online

Oral report Section 3. Modern nuclear physics methods and technologies. Section 3. Modern nuclear physics methods and technologies

Speaker

Vladimir Koltsov (Khlopin Radium Institute, Saint Petersburg, Russia)

Description

The reactor production of the nuclear high-spin isomer ${}^{178m2}$Hf ($T_{1/2}$ = 31 years) was considered. According to [1], in the inelastic scattering of neutrons by ${}^{178}$Hf and in the (n, 2n) reaction by ${}^{179}$Hf, the ${}^{178m2}$Hf isomer is not formed, because this requires the transfer of too large angular momentum to the nucleus. For the formation of the ${}^{178m2}$Hf in the radiative capture of neutrons by ${}^{177}$Hf nuclei, two different cross section values were obtained earlier. In [2] $\sigma$ = 0.2 ± 0.1 $\mu$barn when the ${}^{177}$Hf isotope was irradiated with thermal neutrons with fluence up to $10^{22}$ cm${}^{–2}$. In [3] $\sigma$ = 2.6 ± 0.7 $\mu$barn when neutron irradiating natural hafnium at the IBR-2 reactor of the Joint Institute for Nuclear Research (Dubna) with a relatively small fluence of ~$10^{18}$ cm${}^{–2}$ (the errors are at the level of one standard deviation).
We studied the formation of the ${}^{178m2}$Hf isomer in the material of the regulatory body of the RBT-6 reactor (SSC RIAR), made of 6 mm thick plate of metallic natural hafnium [4], after it's irradiation with neutron flux of ~ $10^{14}$ cm${}^{–2}$∙s${}^{–1}$ with fluence up to $10^{22}$ cm${}^{–2}$. Samples were taken at several points of the plate from the upper layer with a depth of 0.5 mm and from a depth of 2 to 4 mm. The neutron fluence at the sampling points with an accuracy of 20% was determined using a numerical model based on the MCU code (version MCU-RR). For one of the typical sampling points, the fluence of neutrons of energy less than 0.625 eV was 7.5×$10^{21}$ cm${}^{–2}$, the specific activities of the surface and deep samples were 1547 ± 92 Bq×g${}^{–1}$ and 1368 ± 82 Bq×g${}^{–1}$, respectively. If we assume that the whole ${}^{178m2}$Hf isomer was formed by the capture of thermal neutrons by ${}^{177}$Hf nuclei, then taking into account the burn-up of ${}^{177}$Hf and ${}^{178m2}$Hf, the isomer cross section $\sigma$ = 3.6 ± 0.5 $\mu$barn is obtained, which coincides with the result of [3]. Thus, we did not see the contribution of any other reactions to the formation of the ${}^{178m2}$Hf isomer other than radiative capture of neutrons by ${}^{177}$Hf nuclei.
In principle, the ${}^{178m2}$Hf isomers can be produced by the two-stage reaction ${}^{179}$Hf (n, n ’)${}^{179m2}$Hf + ${}^{179m2}$Hf (n, 2n)${}^{178m2}$Hf, which was already discussed in [5] for the interaction of 14 MeV neutrons with ${}^{179}$Hf nuclei. According to our estimates, in the irradiated hafnium studied by us, the specific activity of the ${}^{178m2}$Hf isomer obtained by this reaction is ~ 0.1 Bq×g${}^{-1}$.

  1. S.A.Karamian // Prospects for isomeric energy release. Phys. Part. Nucl. 2008. V.39. P. 490.
  2. R.G.Helmer, C.W.Reich // Nucl. Phys. V. A 211. P. 2. 1973.
  3. S.A.Karamian, J.J.Carroll, J.Adam et al. //. High Energy Density Phys. 2006. V. 2. P. 48. 4. V.D.Risovanyy, E.P.Klochkov, V.B.Ponomarenko // Hafnium in nuclear technology. RIAR. Dimitrovgrad. 1993. 143 P. (in Russian).
  4. M. B.Chadwick, P.G.Young // Nucl. Sci. Engin. 1991. V. 108. P. 117.

Authors

Mr Alexey Izhutov (JSC State Scientific Center - Research Institute of Atomic Reactors) Mr Alexey Petelin (JSC State Scientific Center - Research Institute of Atomic Reactors) Mr Michall Gromov (JSC State Scientific Center - Research Institute of Atomic Reactors) Mr Sergei Sazontov (JSC State Scientific Center - Research Institute of Atomic Reactors) Mr Vasiliy Pimenov (JSC State Scientific Center - Research Institute of Atomic Reactors) Mr Vladimir Afanasiev (JSC State Scientific Center - Research Institute of Atomic Reactors) Vladimir Koltsov (Khlopin Radium Institute, Saint Petersburg, Russia)

Presentation materials