Predictions of 225Ac and 223Ra production cross sections from p, α and heavy ion irradiated thorium and uranium targets

  • 1Advanced Nuclear Energy Team, Advanced Energy Science and Technology Guangdong Laboratory, Huizhou, 516007, China; School of Nuclear Science and Technology, Lanzhou University, Lanzhou, 730000, China.
  • 2Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, 730000, China; Advanced Nuclear Energy Team, Advanced Energy Science and Technology Guangdong Laboratory, Huizhou, 516007, China; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing, 100049, China. Electronic address: zhangyl@impcas.ac.cn.
  • 3School of Nuclear Science and Technology, Lanzhou University, Lanzhou, 730000, China.
  • 4Advanced Nuclear Energy Team, Advanced Energy Science and Technology Guangdong Laboratory, Huizhou, 516007, China.
  • 5Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, 730000, China; Advanced Nuclear Energy Team, Advanced Energy Science and Technology Guangdong Laboratory, Huizhou, 516007, China; School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing, 100049, China.
  • 6Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, 730000, China; Advanced Nuclear Energy Team, Advanced Energy Science and Technology Guangdong Laboratory, Huizhou, 516007, China.

Abstract

-This work studies effective methods for producing 225Ac and 223Ra by bombarding 232Th and natural uranium targets with different incident particles. Direct production of 225Ac via high-energy proton bombardment of 232Th inevitably contains 227Ac impurities, complicating the separation and purification processes. In contrast, obtaining 225Ac through the generated 225Ra can avoid 227Ac contamination. Given the low cross section for the proton-thorium reaction to produce 225Ra, exploring new methods to improve 225Ra production efficiency is critical. This study utilized several physical models of the Monte Carlo transport codes FLUKA and PHITS to calculate the production cross sections of 225Ac, 225Ra, 223Ra, and 227Th via the bombardment of thorium and uranium targets with energetic protons, α-particles, 9Be, and 12C across an energy range of 10-800 MeV/u. The predicted cross sections were then compared with existing experimental data. The predictions indicate that the energy thresholds to produce 225Ac, 225Ra, and 223Ra via α-particle and heavy ion irradiation are lower than those for proton, and the production cross sections are significantly increased, the incident energy corresponding to the peak cross section is mainly below 100 MeV/u. According to the PHITS JQMD-2.0 results, using α-particle bombardment of thorium targets to produce 225Ra and subsequently obtaining high-purity 225Ac may be an efficient production pathway. Moreover, when the α-particle energy is below 100 MeV/u, the predicted cross section of 225Ra for the natural uranium target is higher than that for the thorium target, suggesting that α-particle bombardment of the natural uranium target could be a potential new method to improve 225Ac production efficiency. This study provides theoretical reference for subsequent experimental cross section measurement and isotope production.

Related Concept Videos

Nuclear Transmutation 03:20

17.5K

Nuclear transmutation is the conversion of one nuclide into another. It can occur by the radioactive decay of a nucleus, or the reaction of a nucleus with another particle. The first manmade nucleus was produced in Ernest Rutherford’s laboratory in 1919 by a transmutation reaction, the bombardment of one type of nuclei with other nuclei or with neutrons. Rutherford bombarded nitrogen-14 atoms with high-speed α particles from a natural radioactive isotope of radium and observed...

Types of Radioactivity 03:23

16.7K

The most common types of radioactivity are α decay, β decay, γ decay, neutron emission, and electron capture.
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:

Alpha decay occurs primarily in heavy nuclei (A > 200, Z > 83). Loss of an α particle gives a daughter nuclide with a mass number four units smaller and an atomic number two units smaller than those of the parent nuclide.
Beta...

Biological Effects of Radiation 02:59

15.3K

All radioactive nuclides emit high-energy particles or electromagnetic waves. When this radiation encounters living cells, it can cause heating, break chemical bonds, or ionize molecules. The most serious biological damage results when these radioactive emissions fragment or ionize molecules. For example, α and β particles emitted from nuclear decay reactions possess much higher energies than ordinary chemical bond energies. When these particles strike and penetrate matter, they...

Isotopes and Radioisotopes 01:28

8.5K

In the early 1900s, English chemist Frederick Soddy realized that an element could have atoms with different masses that were chemically indistinguishable. These different types are called isotopes — atoms of the same element that differ in mass. Isotopes differ in mass because they have different numbers of neutrons but are chemically identical because they have the same number of protons. Soddy was awarded the Nobel Prize in Chemistry in 1921 for this discovery.
An isotope containing...

Nuclear Power 02:36

7.7K

Controlled nuclear fission reactions are used to generate electricity. Any nuclear reactor that produces power via the fission of uranium or plutonium by bombardment with neutrons has six components: nuclear fuel consisting of fissionable material, a nuclear moderator, a neutron source, control rods, reactor coolant, and a shield and containment system.
Nuclear Fuels
Nuclear fuel consists of a fissile isotope, such as uranium-235, which must be present in sufficient quantity to provide a...

Radioactive Decay and Radiometric Dating 02:48

33.4K

Radioactivity is a spontaneous disintegration of an unstable nuclide and is a random process, as all the nuclei in the sample do not decay simultaneously. The number of disintegrations per unit time is called the activity (A), which is directly proportional to the number of nuclei in the sample. The decay constant (λ) is an average probability of decay per nucleus in unit time.

The SI unit for activity is the becquerel, which is one disintegration per second. Another unit of activity is the...