New data for $^{52}$Cr and $^{68}$Zn from experiments using bremsstrahlung

5 Jul 2025, 14:30
20m
3058 (Санкт-Петербургский Государственный Университет )

3058

Санкт-Петербургский Государственный Университет

Oral Section 2. Experimental and theoretical studies of nuclear reactions. 2. Experimental and theoretical studies of nuclear reactions

Speaker

Aleksandr Davydov (Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University)

Description

New cross sections of photoneutron reactions $^{52}Cr(\gamma,2n)^{50}Cr$, $^{68}Zn(\gamma,1n)^{67}Zn$ and $^{68}Zn(\gamma,2n)^{66}Zn$ not determined before experimentally were obtained at the first time using the experimental-theoretical method for evaluation of photoneutron partial reaction cross-section meeting physical criteria of reliability method [1]. This method was proposed to solve the problem of significant disagreements between the results of experiments carried out using the beams of quasimonoenergetic annihilation photons and the method for photoneutron multiplicity sorting based on measured neutron energies [2]. Partial reaction cross sections $\sigma^{eval}(\gamma,in) = F_i^{theor} \times \sigma^{exp}(\gamma, xn)$ for $^{52}$Cr and $^{68}$Zn, were evaluated using the experimental yield cross sections $\sigma^{exp}(\gamma,xn) = \sigma^{exp}(\gamma,1n) + 2\sigma^{exp}(\gamma,2n) + 3\sigma^{exp}(\gamma,3n)$ and the ratios $F_i^{theor} = \sigma^{theor}(\gamma,in)/\sigma^{theor}(\gamma,xn)$ calculated for $i = 1, 2, 3$ in Combined photonuclear reaction model (CPNRM) [3]. The published cross sections $\sigma(\gamma,sn) = \sigma(\gamma,1n) + \sigma(\gamma,2n)$ and $\sigma(\gamma,1n)$ for $^{52}$Cr [4] and $\sigma(\gamma,xn)$ for $^{68}$Zn [5] obtained on the beams of bremsstrahlung were used.
It was found that cross sections of reactions $^{52}Cr(\gamma,1n)^{51}Cr$ and ${68}Zn(\gamma,1n)^{67}Zn$ obtained before using the method of introducing statistical theory corrections to the yield cross-section $\sigma^{exp}(\gamma,xn)$ are significantly underestimated, but those of reactions $^{52}Cr(\gamma,2n)^{50}Cr$ and $^{68}Zn(\gamma,2n)^{66}Zn$ overestimated in comparison with evaluated ones and therefore both do not meet physical criteria [6]. The reason is that at photon energies where reactions $(\gamma,1n)$ and $(\gamma,2n)$ compete with each other, the statistical evaporation model became less accurate because processes of the pre-equilibrium decay of a composite system become more important. The CPNRM [3] used in the evaluation method [1] is free from those shortcomings.
New data for cross sections of reactions $^{52}Cr(\gamma,1n)^{51}Cr$, $^{52}Cr(\gamma,2n)^{50}Cr$, $^{68}Zn(\gamma,1n)^{67}Zn$ and $^{68}Zn(\gamma,2n)^{66}Zn$ [6,7] were evaluated in accordance with reliability criteria [1].

  1. V.V. Varlamov et al., Bull. Rus. Acad. Sci. 74, 883 (2010).
  2. V.V. Varlamov et al., Atom. Data and Nucl. Data Tables, 161, 101697 (2025).
  3. B.S. Ishkhanov et al., Phys. Atom. Nucl. 74, 19 (2011).
  4. B.I. Goryachev, et al., Bull. Rus. Acad. Sci. Phys. 33, 1588 (1969).
  5. B.S. Ishkhanov et al., Sov. J. Nucl. Phys. 20, 233 (1975)
  6. V.V. Varlamov et al., Phys. Atom. Nucl. 87, 669 (2024).
  7. V.V. Varlamov et al., Phys. Atom. Nucl. 88 (2025), in print.

Primary authors

Aleksandr Davydov (Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University) Ivan Mostakov (Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University) Vadim Orlin (Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University) Vladimir Varlamov (Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University)

Presentation materials