<p>This study investigates the nuclear structure of Te and Xe isotopes using algebraic collective models. These mid-mass nuclei exhibit collective excitations ranging from spherical vibrations to varying degrees of deformation. Te isotopes are treated as near-spherical or weakly deformed systems and analyzed using the interacting boson model (IBM). The <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1457_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{118}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>118</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Te isotope is described within the U(5) symmetry of the IBM, which represents spherical vibrational behavior. In heavier Te isotopes (<i>A</i> = 120–130), features intermediate between U(5) and O(6) symmetries appear, thereby indicating mixed-mode structures. These are modeled by introducing perturbative contributions from the O(6) Casimir operator into the U(5)-based Hamiltonian. The study also applies Iachello’s critical-point symmetry E(5), which characterizes the phase transition between spherical and <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1457_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation>-soft shapes, to the <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1457_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{128}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>128</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Xe and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1457_Article_IEq4.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\({}^{130}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>130</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Xe isotopes. Calculations of low-lying energy spectra and electromagnetic transition probabilities are used to assess consistency with E(5) symmetry. These results offer new insights into shape evolution in mid-mass nuclei and highlight the effectiveness of algebraic models in describing nuclear phase transitions.</p>

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Structure analysis of tellurium and xenon nuclei according to mass number using algebraic models

  • Su Youn Lee

摘要

This study investigates the nuclear structure of Te and Xe isotopes using algebraic collective models. These mid-mass nuclei exhibit collective excitations ranging from spherical vibrations to varying degrees of deformation. Te isotopes are treated as near-spherical or weakly deformed systems and analyzed using the interacting boson model (IBM). The \({}^{118}\) 118 Te isotope is described within the U(5) symmetry of the IBM, which represents spherical vibrational behavior. In heavier Te isotopes (A = 120–130), features intermediate between U(5) and O(6) symmetries appear, thereby indicating mixed-mode structures. These are modeled by introducing perturbative contributions from the O(6) Casimir operator into the U(5)-based Hamiltonian. The study also applies Iachello’s critical-point symmetry E(5), which characterizes the phase transition between spherical and \(\gamma\) γ -soft shapes, to the \({}^{128}\) 128 Xe and \({}^{130}\) 130 Xe isotopes. Calculations of low-lying energy spectra and electromagnetic transition probabilities are used to assess consistency with E(5) symmetry. These results offer new insights into shape evolution in mid-mass nuclei and highlight the effectiveness of algebraic models in describing nuclear phase transitions.