Effective valence proton numbers for nuclei with Z{approx}64

The subshell effect for nuclei with proton number Z{approx} 64 has been known for many years. The most economic way to consider this effect is to use the effective valence proton number. In this Brief Report we extract effective valence proton numbers for nuclei in this region by using the systematics of the first 2{sup +} energies (E{sub 21}{sup +}) of even-even nuclei, the ratios of the first 4{sup +} and 6{sup +} state energies with respect to E{sub 21}{sup +} (R{sub 4} and R{sub 6}), the B(E2) values, the quadrupole deformation parameters e{sub 2}, and anomalous g factors of the 2{sub 1}{sup +} state for even-even nuclei. It is noticed that these physical quantities saturate when N{sub p}N{sub n}, the product of the valence proton number and the valence neutron number, is large enough; on the other hand, they go to saturation at different ''speeds.'' We show that the subshell effect is more evident for E{sub 21}{sup +} and yrast state energy ratios (R{sub 4} and R{sub 6}), and relatively less for other quantities.

[1]  J. K. Hwang,et al.  g factors of first 2 + states of neutron-rich Xe, Ba, and Ce isotopes , 2009 .

[2]  J. Yoon,et al.  NpNn Scheme and the Valence Proton-Neutron Interaction , 2008, 0805.2790.

[3]  J. Yoon,et al.  NpNn dependence of empirical formula for the lowest excitation energy of the 2+ states in even–even nuclei , 2007, 0711.3802.

[4]  J. Yoon,et al.  NpNn scheme based on new empirical formula for excitation energy , 2007, 0704.1693.

[5]  N. Stone Table of Nuclear Magnetic Dipole and Electric Quadrupole Moments , 2005 .

[6]  A. H. Wapstra,et al.  The AME2003 atomic mass evaluation . (II). Tables, graphs and references , 2003 .

[7]  A. Arima,et al.  Systematics of nuclear deformation in large regions , 2001 .

[8]  Zhao,et al.  Generalization of the N(p)N(n)N(p)N(n) scheme and the structure of the valence space , 2000, Physical review letters.

[9]  R. Casten,et al.  TOPICAL REVIEW: The evolution of nuclear structure: the ? scheme and related correlations , 1996 .

[10]  Zhao,et al.  Regional regularities for the even-even nuclei: Medium to heavy systems. , 1995, Physical review. C, Nuclear physics.

[11]  W. Myers,et al.  Nuclear ground state masses and deformations , 1993, nucl-th/9308022.

[12]  Zamfir,et al.  Valence correlation schemes and signatures of nuclear structure: A simple global phenomenology for B(E2:21+-->01+) values. , 1993, Physical review letters.

[13]  Han,et al.  Effective boson number calculations near the Z=64 subshell. , 1990, Physical review. C, Nuclear physics.

[14]  A. Arima,et al.  The Interacting Boson Model: The interacting boson model-2 , 1987 .

[15]  R. Casten NpNn systematics in heavy nuclei , 1985 .

[16]  N. Benczer-koller,et al.  Effective g factors and proton-boson numbers in the vicinity of proton subshell closures , 1985 .

[17]  Casten Possible unified interpretation of heavy nuclei. , 1985, Physical review letters.

[18]  S. T. Hsieh,et al.  STRUCTURES OF N=88 AND N=90 ISOTONES IN THE INTERACTING BOSON APPROXIMATION , 1984 .

[19]  O. Scholten ON THE EFFECTIVE NUMBER OF BOSONS IN THE INTERACTING BOSON MODEL , 1983 .

[20]  Francesco Iachello,et al.  Interacting boson model , 1981 .

[21]  D. S. Brenner,et al.  Relation between the Z = 64 Shell Closure and the Onset of Deformation at N = 88 − 90 , 1981 .

[22]  S. Pittel,et al.  Towards a unified microscopic description of nuclear deformation , 1977 .

[23]  A. Arima,et al.  COLLECTIVE NUCLEAR STATES AS REPRESENTATIONS OF A SU(6) GROUP , 1975 .

[24]  I. Talmi EFFECTIVE INTERACTIONS AND COUPLING SCHEMES IN NUCLEI , 1962 .

[25]  M. Goldhaber,et al.  Mixed Configurations in Nuclei , 1953 .