共查询到18条相似文献,搜索用时 156 毫秒
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本文提出了一个处理原子核中nn及pp对力的近似方法。这个方法避免了通常将BCS-Боголюбов方法应用于原子核所引起的困难,例如粒子数不守恒,假态的出现以及不同激发态波函数不正交等。但这个方法只有在所需考虑的粒子数n及能级数Ω不太大时(n≤10,Ω≤10)才能较方便地被应用,近似程度才比较好。在这个方法中,毋须引入准粒子的概念,激发的多体性质被明显地表示出来。系统的激发可分为两大类型。第一类型激发是一种以多体系为背景的单粒子跃迁,相应于一个准粒子的跃迁αv+αv,或两个准粒子的激发αv+βv′+,αv+αv′+(v≠v′)。第二类型激发是对激发,在这种激发中,各能级上共轭粒子对的填充几率改变了,相应于共轭的准粒子对的激发αv+βv+,αv+βv+αμ+βμ+,….本文还考察了对力在r及β跃迁中的影响。在β跃迁中,对力一般是使跃迁受阻。在r跃迁中,对力的效应随初末态间的相对激发类型不同而异,如相对激发属于第一类型,则跃迁受阻,受阻程度随跃迁的电磁性质不同而有所差别,如相对跃迁属于第二类型,则在无对力作用时跃迁是禁戒的,在对力作用下也只有由电荷电流所产生的电跃迁是允许的。最后本文以Hf178为例,应用上述方法,初步分析了对力对偶偶核的内部激发能谱及β衰变的影响。 相似文献
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刘忠 张玉虎 郭应祥 周小红 雷相国 柳敏良 罗万居 何建军 郑勇 潘强岩 甘再国 罗亦孝 T.Hayakawa M.Oshima Y.Toh T.Shizima Y.Hatsukawa A.Osa T.Ishii M.Sugawara 《中国物理 C》2002,26(10):1015-1020
利用420MeV82Se轰击139La引起的深部非弹反应和在束γ谱学方法研究了142Ce的中高自旋激发态.识别出了激发能为2625,2995和3834keV的3个新能级,自旋、宇称分别被指定为8+,9(-)和11(-).发现这些能级非常好地符合N=84偶偶核转晕能级的系统性.利用经验壳模型计算了142Ce的中高自旋激发态的激发能,计算结果比较好地重现了实验值.对它们的结构进行了讨论,表明在142Ce的中高自旋激发态中以单粒子激发为主 相似文献
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采用修正的表面δ相互作用(MSDI),对102—114Ru,102—116Pd和104—116Cd等22个偶偶核分别在gds和gdsh两种不同的组态空间中作了形变HF计算.得到了长、扁椭球等基态或激发态的解.结果表明在质量数为102—116间的原子核存在形状过渡和形状共存现象,且单粒子能级随质量数及组态的不同而不同.两种不同组态空间中的计算结果的对比表明,形变HF计算中1h11/2轨道的介入及填充与否对A~100区偶偶核的单粒子能谱及形状有较大影响 相似文献
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在210MeV的束流能量下, 利用重离子熔合蒸发反应146Nd(35Cl, 5nγ)176Ir产生具有β+/EC衰变性质的核素176Ir,由氦喷嘴快速带传输系统将反应产物传送到低本底区进行测量. 经过实验数据的离线处理分析,对早先发表的176Ir衰变γ跃迁进行确认的同时又发现了3个新能级和10条新的γ射线, 丰富了176Os核的低位激发态能级纲图. 并根据典型γ射线的衰变时间谱建议了176Ir核的一个长寿命的低自旋同核异能态. 相似文献
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By using a simple barrier penetration approach,we predict the α-decay branching ratios to members of ground-state rotational band of heavy even-even No isotopes.We also extend our approach to calculate the α-decay branching ratios to the rotational band of heavy odd-A nuclei.The theoretical branching ratios of α-decays are found in good agreement with the available experimental data. 相似文献
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N. Buforn A. Astier J. Meyer M. Meyer S. Perriès N. Redon O. Stézowski M.G. Porquet I. Deloncle A. Bauchet J. Duprat B.J.P. Gall C. Gautherin E. Gueorguieva F. Hoellinger T. Kutsarova R. Lucas A. Minkova N. Schulz H. Sergolle Ts. Venkova A.N. Wilson 《The European Physical Journal A - Hadrons and Nuclei》2000,7(3):347-353
High-spin states in 113-116Cd have been investigated with the fusion-fission reaction 28Si +176Yb at 145 > MeV. The experiment has been performed with the Eurogam2 array. New rotational bands based on two quasi-particle
states have been observed for even-even cadmium isotopes. A new level scheme based on the 11/2− isomeric state is proposed for 115Cd and the one of 113Cd has been extended to spin (31/2−). The decoupled bands identified in both odd-A nuclei are interpreted as being built upon a low-Ωh11/2 quasi-neutron configuration. Microscopic Hartree-Fock + BCS calculations confirm the prolate deformation in this mass region
especially for the odd cadmium isotopes.
Received: 21 December 1999 / Revised version: 16 February 2000 相似文献
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B. S. Ishkhanov M. E. Stepanov T. Yu. Tretyakova 《Moscow University Physics Bulletin》2014,69(1):1-20
The nucleon pairing effect that is analyzed in the present paper is one of the striking manifestations of nuclear dynamics. Nucleon pairing for different chains of nuclei dependent upon the number of protons or neutrons in the nucleus allows one to explain the emergence of a great number of positive-parity states, which form a ground state multiplet, in even-even nuclei in the excitation energy range E* < 4 MeV. The interaction of paired nucleons with vibrational and rotational degrees of freedom of a nucleus produces a wide variety of excitation spectra of positive-parity states in even-even nuclei. 相似文献
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A. N. Kuzmina G. G. Adamian N. V. Antonenko 《Bulletin of the Russian Academy of Sciences: Physics》2013,77(4):406-410
The one-quasiparticle structures of nuclei in the α-decay chains of 287114 and 293116 are studied using a modified two-center shell model. Two-quasiparticle states are revealed in the α-decay chain of even-even nuclei 286,288114. The calculated values for Q α are compared to the available experimental data. The termination of the α-decay chains by spontaneous fission is analyzed. 相似文献
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By fitting the E2 transition spectra of superdeformed bands in A~190 region, the coefficients of Bohr-Mottelson's I(I+1) expansion are determined and moments of inertia of band head are calculated out. All results show that the moments of inertia of odd-A nuclei are systematically larger than those of the neighboring even-even nuclei, and the moments of inertia of odd-odd nuclei are systematically larger than those of the neighboring odd-A nuclei. The odd-even difference of moment of inertia of nuclear superdeformed states is obvious. 相似文献
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In this work,β~+/EC decays of some medium-mass nuclei are investigated within the extended quasiparticle random-phase approximation(QRPA),where neutron-neutron,proton-proton and neutron-proton(np) pairing correlations are taken into consideration in the specialized Hartree-Fock-Bogoliubov(HFB) transformation.In addition to the pairing interaction,the Br¨uckner G-matrix obtained with the charge-dependent Bonn nucleon-nucleon force is used for the residual particle-particle and particle-hole interactions.Calculations are performed for even-even proton-rich isotopes ranging from Z =24 to Z =34.It is found that the np pairing interaction plays a significant role inβ-decay for some nuclei far from stability.Compared with other theoretical calculations,our calculations show good agreement with the available experimental data.Predictions of β-decay half-lives for some very neutron-deficient nuclei are made for reference. 相似文献
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《Nuclear Physics A》1998,643(1):39-51
The projected shell model is a shell-model theory built up over a deformed BCS mean field. Ground state and excited bands in even-even nuclei are obtained through diagonalization of a pairing plus quadrupole Hamiltonian in an angular momentum projected 0-, 2-, and 4-quasiparticle basis. The residual quadrupole-quadrupole interaction strength is fixed self-consistently with the deformed mean field and the pairing constants are the same used in constructing the quasiparticle basis. Taking 160Dy as an example, we calculate low-lying states and compare them with experimental data. We exhibit the effect of changing the residual interaction strengths on the spectra. It is clearly seen that there are many Jπ = 0+, 1+, 4+ bandheads whose energies can only be reproduced using the self-consistent strengths. It is thus concluded that the projected shell model is a model with essentially no free parameters. The predicted energy of the 2+ bandhead lies however in nearly twice the experimental value. 相似文献