Three interesting characteristics of the octupole deformed Yrast bands in even-even nuclei can be reproduced in the framework of our model.
2低自旋区存在宇称劈裂，负宇称态的位置相对于相邻正宇称态的平均位置较高。
The variations in moments of inertia J(2 and J(1) with rotational frequency for the series of yrast SD bands in even-even nuclei, 192—198 Pb(1) and 198 Po(1), are investigated by using the particle-number conserving method for treating the pairing interaction.
用处理对力的粒子数守恒方法分析了A～190区偶偶核系列晕SD带192—198Pb(1)和198Po(1)的转动惯量随角频率变化的规律。计算中同时考虑了单极对力与Y20四极对力。
A Microscopic Two-Parameter Nuclear Model and Its Application to the Yrast Lines of Actinide Nuclei
一个微观两参数核模型和它对超铀区核Yrast线的应用
A two-parameter model based on the microscopic fermion dynamical symmetry model is proposed. In terms of the numerical calculation, it is shown that this model can fit the data of the yrast lines of nuclei in the actinide region in very high precision.
基于费米子动力学对称模型提出了一个两参数模型.数值计算显示此模型能很好地符合超铀区核Yrast线能谱。
Structural Evolution in the Yrast-band of~(72) Kr Nuclei within Microscopic Theory
~（72）Kr核中yrast带结构演化的微观研究
Observation and Empirical Shell-Model Study of New Yrast Excited States in the Nucleus~(142) Ce
~（142）Ce的新激发态及其经验壳模型研究
Calculation of Yrast Bands for Odd-Odd Nuclei~(80, 82) Rb in A ≈ 80 Mass Region
A≈80区奇-奇核~（80,82）Rb的晕带能谱计算
Yrast Band and Four - Quasiparticle Band in Odd-Odd - (162) Lu Nucleus
奇奇核￣（162）Lu晕转带及四准粒子带的能级结构
A possible explanation of the double backbending of YRAST band for nuclei~(122, 124, 126) te
~（122124126）Te的双回弯的一种可能解释
A phenomenological description of YRAST STATES in the even even xenon, barium AND CERIUM ISOTOPES
对偶偶氙、钡、铈同位素核Yrast态的一种唯象描述
It has been identified that the quantum phase transitions from the vibrational ground-state phase to rotational one occupy in the yrast-band of 76Sr nuclei, according to the -ray energy over spin curves, and based on the microscopic sdIBM-2 approach and the single-particle energies from experiment, one has reproduced successfully by same equal parameters except for K, after that we had fined a particular real example that in order to take place one only to need adjust the K parameter enough.
射线能量-自旋曲线分析方法指认：76Sr核的yrast带存在从振动基态相到转动基态相的基态量子相变。借助微观sdIBM-2方案和实验单粒子能量值，用了除外，完全相同的一组参数成功地再现了它们相应的基态量子相变，找到了只需要单独调整中子-质子相互作用强度就能实现基态相变的特殊实例。
And phenomenological study identifies that: 1 The coexisting region of two excitation models is on the interval between the state 8(superscript + subscript 1) and state 14(superscript + subscript 1) this is a interval with E(subscript x=3.683-5.503 MeV, and the 8(superscript + subscript 1) state is a state preponderant in the vibrational model, the 14(superscript + subscript 1) state is one predominant in the rotational model, while the state 10(superscript + subscript 1) is a crossbencher state relative to the two models; 2 The yrast states from the ground-state up to the 24(superscript + subscript 1) state all are collective states, hereafter the first breaking up and aligning state maybe is a two-quasiparticle state of neutron on the intruder orbits h(subscript 1/23 This structure evolution has been achieved via the moderate changes of the pair coupling probability of valence nucleons in the coexisting region, and thus is not very rapidly.
微观和唯象的研究指出：1这两种激发模式的共存区是能态81(上标+下标 1)4(上标+下标 1)E(下标 x=3.683~5.503 MeV，8(上标+下标 1)态是振动模式占据优势的能态，14(上标+下标 1)态是转动模式占据优势的能态，而10(上标+下标 1)态则是两种模式的中立能态；2从基态到24(上标+下标 1)态的yrast态均是集体态，而以后出现的第1个拆对顺排态很可能就是中子h(下标 11/2)的两准粒子态；3核结构的这种过渡不是很剧烈，而是在过渡区中，通过对玻色子结构中价核子对的耦合概率的微小改变来实现的。
On the mechanism of signature inversion in the yrast band of~(84) Rb
~（84）Rb晕带signature反转的机理
Microscopic Mechanism of the ω Variation in Moments of Inertia for Yrast SD Bands~(194) T1
~（194）T1奇-奇超形变带转动惯量变化的微观机制
Microscopic calculations of the YRAST superdeformed bands of the even even nuclei in the A~190 mass region
A～190区偶偶核超形变晕带能谱的微观计算
A New Formula for the Spectra of Axial Symmetric and Transition Nuclei and a Quantity to Identify the Nuclear γ Deformation
一个描述轴对称、过渡核yrast带的新公式及核γ形变的一个特征量
Level density just above YRAST line
转晕线上的能级密度
A possible explanation of the double backbending of YRAST band for nuclei ~ (122,124,126) te
~（122124126）Te的双回弯的一种可能解释