论文标题

在$^{35} $ p中搜索$ 1/2^+$入侵状态

Search for the $1/2^+$ intruder state in $^{35}$P

论文作者

Salathe, M., Crawford, H. L., Macchiavelli, A. O., Kay, B. P., Hoffman, C. R., Ayangeakaa, A. D., Campbell, C. M., Clark, R. M., Cromaz, M., Fallon, P., Jones, M. D., Kuvin, S. A., Sethi, J., Wiedeking, M., Winkelbauer, J. R., Wuosmaa, A. H.

论文摘要

变形的入侵态的激发能(特别是2P2H带头)作为质子数量$ z $沿$ n = 20 $的函数,这既令人感兴趣,这既是更好地理解核结构的演变,而在该区域中,将球形$^{40} $ CA与逆转核岛之间的核结构演变为基础。在$ n = 20 $倒置的中心,NPNH(其中n = 2,4,6)中子激发$ n = 20 $差距导致变形和集体基态,如$^{32} $ mg所示。在较重的同位酮中,NPNH激发在接地状态下不占主导地位,而是存在于相对较低的水平方案中。目的是确定预期的2p2h $ \ otimes \ mathrm {s} _ {1/2^+} $状态$^{35} $ p,唯一的$ n = 20 $ n = 20 $ sotone neutron 2p2h兴奋bandhead尚未确定$^36} $^$^$^3 $^3 $^3 $^3 $^3 $^3 $^3 $^3 $^3,$^3 $^3 $^3 $^3,$^3,$^3 $^3 $^3,$^3 $^3,$^3 $^3,$^3 $^3,He)在Argonne Tandem Linac Accelerator系统(ATLAS)的螺旋轨道光谱仪(Helios)的逆运动学中。虽然尚未找到候选状态,但转移反应横截面的上限将在2.5至3.6 \内填充这种配置的MEV能量范围内,对两个$^{36} $ s和$^{35} $ p的波函数组合物提供了严格的约束。

The excitation energy of deformed intruder states (specifically the 2p2h bandhead) as a function of proton number $Z$ along $N=20$ is of interest both in terms of better understanding the evolution of nuclear structure between spherical $^{40}$Ca and the Island of Inversion nuclei, and for benchmarking theoretical descriptions in this region. At the center of the $N=20$ Island of Inversion, the npnh (where n=2,4,6) neutron excitations across a diminished $N=20$ gap result in deformed and collective ground states, as observed in $^{32}$Mg. In heavier isotones, npnh excitations do not dominate in the ground states, but are present in the relatively low-lying level schemes. With the aim of identifying the expected 2p2h$\otimes\mathrm{s}_{1/2^+}$ state in $^{35}$P, the only $N=20$ isotone for which the neutron 2p2h excitation bandhead has not yet been identified, the $^{36}$S(d,$^3$He)$^{35}$P reaction has been revisited in inverse kinematics with the HELical Orbit Spectrometer (HELIOS) at the Argonne Tandem Linac Accelerator System (ATLAS). While a candidate state has not been located, an upper limit for the transfer reaction cross-section to populate such a configuration within a 2.5 to 3.6\,MeV energy range, provides a stringent constraint on the wavefunction compositions in both $^{36}$S and $^{35}$P.

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