Photodisintegration of Palladium Isotopes

Белышев, С. С.; Ishkhanov, B. S.; Кузнецов, А. А.; Orlin, V. N.; Prosnyakov, A.; Fursova, N. Yu.; Khankin, V. V.

doi:10.3103/s0027134920060065

Cited by 4 publications

(1 citation statement)

References 45 publications

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“…For the yield measurement for a natural mixture of isotopes the result is the yield of isotope production in all possible reactions on a The main disadvantage of beam experiments bremsstrahlung is that the yield of photonuclear reaction depends both on the studied cross section of the reaction σ(E) and the shape of the bremsstrahlung spectrum W(E, E γmax ), which is often known with insufficient accuracy. That's why the data obtained from the photonuclear experiment on bremsstrahlung beams are generally represented in terms of the relative yields or the integrated reaction cross section [33][34][35], the flux weighted average cross section <σ> [36][37][38][39][40][41][42][43], or the cross section per equivalent photon σ q [35,37,43,44].…”

Section: Resultsmentioning

confidence: 99%

Photonuclear reactions on stable isotopes of selenium at bremsstrahlung end-point energies of 10−23 MeV

Rasulova,

Aksenov,

Alekseev

et al. 2024

Chinese Phys. C

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The experiments were performed at bremsstrahlung end-point energies of 10-23 MeV with the beam from the MT-25 microtron with the use of the γ-activation technique. The experimental values of relative yields were compared with theoretical results obtained on the basis of TALYS with the standard parameters and the combined model of photonucleon reactions. Including isospin splitting in the combined model of photonucleon reactions allows to describe experimental data on reactions with proton escape in energies range from 10 to 23 MeV. Therefore, taking into account isospin splitting is necessary for a correct description of the decay of the GDR.

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