Abstract <p>It is shown that, using published results from various experiments performed with bremsstrahlung <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <!--BPhysMGU2670023Varlamov-m3--> </InlineEquation>-radiation beams, it is in many cases possible to obtain new data on photodisintegration of nuclei, primarily cross sections of photoneutron reactions, which were previously unknown. Such possibilities have been realized for the nuclei <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({}^{52}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m4--> </InlineEquation>Cr and <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m5--> </InlineEquation>Zn. Previously unpublished cross sections <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\sigma(\gamma,2n)\)</EquationSource> <!--BPhysMGU2670023Varlamov-m6--> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\sigma(\gamma,xn)=\sigma(\gamma,1n)+2\sigma(\gamma,2n)\)</EquationSource> <!--BPhysMGU2670023Varlamov-m7--> </InlineEquation> for the nucleus <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({}^{52}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m8--> </InlineEquation>Cr, and <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\sigma(\gamma,1n)\)</EquationSource> <!--BPhysMGU2670023Varlamov-m9--> </InlineEquation>, <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\sigma(\gamma,2n)\)</EquationSource> <!--BPhysMGU2670023Varlamov-m10--> </InlineEquation> and <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\sigma(\gamma,sn)=\sigma(\gamma,1n)+\sigma(\gamma,2n)\)</EquationSource> <!--BPhysMGU2670023Varlamov-m11--> </InlineEquation> for the nucleus <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m12--> </InlineEquation>Zn have been obtained for the first time based on published experimental data. It has been established that the experimental cross sections of partial reactions on the <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\({}^{52}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m13--> </InlineEquation>Cr nucleus do not satisfy objective physical reliability criteria. New cross sections for the reactions <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\({}^{52}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m14--> </InlineEquation>Cr(<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\gamma,1n\)</EquationSource> <!--BPhysMGU2670023Varlamov-m15--> </InlineEquation>) and <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\({}^{52}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m16--> </InlineEquation>Cr(<InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\gamma,2n\)</EquationSource> <!--BPhysMGU2670023Varlamov-m17--> </InlineEquation>)<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\({}^{50}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m18--> </InlineEquation>Cr, which meet physical criteria, have been evaluated using an experimental–theoretical method and used to determine a new cross section for the total photoneutron reaction <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\({}^{52}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m19--> </InlineEquation>Cr(<InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\gamma,sn\)</EquationSource> <!--BPhysMGU2670023Varlamov-m20--> </InlineEquation>). In the case of the <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m21--> </InlineEquation>Zn nucleus, using the only published experimental cross section for neutron yield <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m22--> </InlineEquation>Zn(<InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(\gamma,xn\)</EquationSource> <!--BPhysMGU2670023Varlamov-m23--> </InlineEquation>), new previously unknown cross sections of partial reactions <InlineEquation ID="IEq24"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m24--> </InlineEquation>Zn(<InlineEquation ID="IEq25"> <EquationSource Format="TEX">\(\gamma,1n\)</EquationSource> <!--BPhysMGU2670023Varlamov-m25--> </InlineEquation>)<InlineEquation ID="IEq26"> <EquationSource Format="TEX">\({}^{67}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m26--> </InlineEquation>Zn and <InlineEquation ID="IEq27"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m27--> </InlineEquation>Zn(<InlineEquation ID="IEq28"> <EquationSource Format="TEX">\(\gamma,2n\)</EquationSource> <!--BPhysMGU2670023Varlamov-m28--> </InlineEquation>)<InlineEquation ID="IEq29"> <EquationSource Format="TEX">\({}^{66}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m29--> </InlineEquation>Zn, as well as the cross section of the total photoneutron reaction <InlineEquation ID="IEq30"> <EquationSource Format="TEX">\({}^{68}\)</EquationSource> <!--BPhysMGU2670023Varlamov-m30--> </InlineEquation>Zn(<InlineEquation ID="IEq31"> <EquationSource Format="TEX">\(\gamma,sn\)</EquationSource> <!--BPhysMGU2670023Varlamov-m31--> </InlineEquation>), have been obtained for the first time using the experimental–theoretical method.</p>

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New Data on Photodisintegration of Atomic Nuclei from Results of Experiments with Bremsstrahlung \({\gamma}\)-Radiation Beams

  • V. V. Varlamov,
  • A. I. Davydov,
  • V. N. Orlin

摘要

Abstract

It is shown that, using published results from various experiments performed with bremsstrahlung \(\gamma\) -radiation beams, it is in many cases possible to obtain new data on photodisintegration of nuclei, primarily cross sections of photoneutron reactions, which were previously unknown. Such possibilities have been realized for the nuclei \({}^{52}\) Cr and \({}^{68}\) Zn. Previously unpublished cross sections \(\sigma(\gamma,2n)\) and \(\sigma(\gamma,xn)=\sigma(\gamma,1n)+2\sigma(\gamma,2n)\) for the nucleus \({}^{52}\) Cr, and \(\sigma(\gamma,1n)\) , \(\sigma(\gamma,2n)\) and \(\sigma(\gamma,sn)=\sigma(\gamma,1n)+\sigma(\gamma,2n)\) for the nucleus \({}^{68}\) Zn have been obtained for the first time based on published experimental data. It has been established that the experimental cross sections of partial reactions on the \({}^{52}\) Cr nucleus do not satisfy objective physical reliability criteria. New cross sections for the reactions \({}^{52}\) Cr( \(\gamma,1n\) ) and \({}^{52}\) Cr( \(\gamma,2n\) ) \({}^{50}\) Cr, which meet physical criteria, have been evaluated using an experimental–theoretical method and used to determine a new cross section for the total photoneutron reaction \({}^{52}\) Cr( \(\gamma,sn\) ). In the case of the \({}^{68}\) Zn nucleus, using the only published experimental cross section for neutron yield \({}^{68}\) Zn( \(\gamma,xn\) ), new previously unknown cross sections of partial reactions \({}^{68}\) Zn( \(\gamma,1n\) ) \({}^{67}\) Zn and \({}^{68}\) Zn( \(\gamma,2n\) ) \({}^{66}\) Zn, as well as the cross section of the total photoneutron reaction \({}^{68}\) Zn( \(\gamma,sn\) ), have been obtained for the first time using the experimental–theoretical method.