In the doubly magic nucleus \(^{208}\mathrm{Pb}\) states at excitation energies \(6\,\lesssim \, E_x <7.0\) MeV populated by the inelastic proton scattering via the doublet isobaric analog resonances g \(_{{ 7}/{2}}\)+d \(_{{ 3}/{2}}\) in \(^{209}\mathrm{Bi}\) are studied. Sixteen states containing dominant strengths of the configurations g \(_{{ 7}/{2}}\)p \(_{{ 3}/{2}}\), d \(_{{ 3}/{2}}\)p \(_{{ 3}/{2}}\), g \(_{{ 7}/{2}}\)f \(_{{ 5}/{2}}\), d \(_{{ 3}/{2}}\)f \(_{{ 5}/{2}}\) are newly assigned spins from \(2^-\) to \(6^-\), among them ten states are newly identified. Amplitudes with relative signs of up to four one-particle one-hole configurations with strengths down to 0.05% are determined in 40 states with spins from 1\(^-\) to \(6^-\). Amplitudes of configurations d \(_{{ 3}/{2}}\)p \(_{{ 1}/{2}}\), d \(_{{ 3}/{2}}\)p \(_{{ 3}/{2}}\), d \(_{{ 3}/{2}}\)f \(_{{ 5}/{2}}\) for fourteen states and amplitudes of g \(_{{ 7}/{2}}\)p \(_{{ 1}/{2}}\), g \(_{{ 7}/{2}}\)p \(_{{ 3}/{2}}\), g \(_{{ 7}/{2}}\)f \(_{{ 5}/{2}}\) for twenty-seven states are determined. Total strengths up to the full strength are found for configurations d \(_{{ 3}/{2}}\)p \(_{{ 1}/{2}}\), d \(_{{ 3}/{2}}\)p \(_{{ 3}/{2}}\), d \(_{{ 3}/{2}}\)f \(_{{ 5}/{2}}\) with spins from \(1^-\) to \(3^-\) and for g \(_{{ 7}/{2}}\)p \(_{{ 1}/{2}}\), g \(_{{ 7}/{2}}\)p \(_{{ 3}/{2}}\), g \(_{{ 7}/{2}}\)f \(_{{ 5}/{2}}\) with spins from 1\(^-\) to \(6^-\).

中文翻译：

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负奇偶校验状态的结构为$$ {\ mathbf {6} \，\ lesssim \，\ mathbf {E} _ \ mathbf {x} <{\ mathbf {7.0}}} $$ 6 E x <7.0 MeV in $$ \ mathbf {^ {208}} {} \ mathbf {Pb} $$ 208 Pb

在双魔核\（^ {208} \ mathrm {Pb} \）的激发能量\（6 \，\ lesssim \，E_x <7.0 \）的状态下，  MeV由经由双重等压模拟共振g 的非弹性质子散射构成研究了\（^ {209} \ mathrm {Bi} \）中的\（_ {{7} / {2}} \） + d \（_ {{3} / {2}} \）。包含配置g的主导强度的16个状态g \（_ {{7} / {2}} \）p \（_ {{3} / {2}} \），d \（_ {{3} / {2 }} \）p \（_ {{3} / {2}} \），g \（_ {{7} / {2}} \）f \（_ {{5} / {2}} \），d \（_ {{3} / {2}} \） f \（_ {{5} / {2}} \）是从\（2 ^-\）到\（6 ^-\）的新分配的自旋，其中新识别了十个状态。在40种状态下，自旋从1 \（^-\）到\（6 ^-\），确定相对符号最多为四个单粒子单孔构型的强度（强度低至0.05％）。配置幅度d \（_ {{3} / {2}} \）p \（_ {{1} / {2}} \），d \（_ {{3} / {2}} \）p \（_ {{3} / {2}} \），d \（_ {{3} / {2}} \）f \（_ {{5} / {2}} \）对于十四个状态和振幅的g \（_ {{7} / {2}} \）p \（_ {{1} / {2}} \），g \（_ {{7} / {2}} \）p \（_ {{3} / {2}} \），g \（_确定了27个状态的{{7} / {2}} \）f \（_ {{5} / {2}} \）。找到配置d \（_ {{3} / {2}} \）p \（_ {{1 1 / {2}} \），d \（_ {{3} / {2}} \）p \（_ {{3} / {2}} \），d \（_ {{3} / {2}} \）f \（_ {{5} / {2} } \）从\（1 ^-\）到\（3 ^-\）旋转，对于g \（_ {{7} / {2}} \）p \（_ {{1} / {2} } \），g \（_ {{7} / {2}} \）p \（_ {{3} / {2}} \），g \（_ {{7} / {2}} \）f \（_ { {5} / {2}} \）从1 \（^-\）旋转到\（6 ^-\）。