2) Doubly excited state
双激发态
1.
Energies of doubly excited states 1s~22pnd~1P_1~0(n=3～50) of beryllium atom;
铍原子1s~22pnd~1P_1~0(n=3-50)双激发态能级的计算(英文)
3) Highly-excited state
高激发态
1.
We caculated the highly-excited states with J =1 and odd parity of the Beryllium isoelectronic sequence by using the eigenchannel quantum defect theory (EQDT).
应用本征通道量子亏损理论（ＥＱＤＴ），计算了类Ｂｅ原子体系（Ｂｅ－ＭｇⅨ）的高激发态结构（奇宇称，Ｊ＝１），得到了表征高激发态性质的ＥＱＤＴ参量及２ｐｎｓ，２ｐｎｄ和２ｓｎｐ组态的全部Ｒｙｄｂｅｒｇ能级位置及通道混合系数。
2.
We calculated the highly-excited states with J = 0, 1 and 2 and even parity of the beryllium isoelectronic sequence by using the eigenchannel quantum defect theory (EQDT).
本文应用本征通道量子亏损理论(EQDT)系统地研究了J=0,1,2,偶宇称Be等电子序列(BeI—SiⅪ)的高激发态结构。
3.
On the basis of the eigenchannel quantum defect theory (EQDT) we calculated the highly-excited state structure of 3sns (J= 0) Rydberg series for the ionic A1 (?) .
本文利用本征通道量子亏损理论方法计算了一价铝离子3sns(J=0)里德伯系列的激发态结构,给出了高激发态结构的具体数值结果,并讨论了干状态的影响。
4) highly excited state
高激发态
1.
Calculation of energy levels of alkali-metal-atoms highly excited states by using Hammerling exchange potential;
用Hammerling交换势计算碱金属原子高激发态能级
2.
A new phenomenological potential for highly excited states of alkali metal atom is suggested.
对碱金属原子的高激发态提出了一个新的唯象势，并用ＰＷＫＢ法给出了量子亏损（因而能级）的计算公式。
3.
The investigation of highly excited states of the rare-earth atom is not only an important subject in the atomic physics, astrophysics and plasmas, but also helpful for the related scientific and technical fields, such as laser isotope separate, development of new laser and lasing without population inversion etc.
开展稀土元素高激发态的研究不仅是原子物理学、天体物理学、等离子体物理学等领域的重要课题,而且在许多高科技领域也有广泛的应用价值,如激光分离同位素、新型激光器的开发以及自电离无反转光放大等。
5) the most intensive structure
最高激发态
1.
In this paper, the most intensive structure proposed first in Hierarchical-Structure (H-S) model is further studied, and it is concluded that there exists an absolute scaling law for this structure, and the statistical absolute scaling behavior is only produced by the local and strong intermittence structure.
通过对湍流层次结构模型中提出的最高激发态的进一步研究发现,最高激发态存在绝对标度律,且该绝对标度律是由信号中最强耗散涨落的局部结构产生的,并由此推测出局部强间歇结构一般具有绝对标度的结论。
6) DOuble excited state
球对称双激发态
补充资料：[(9,10-二氢-9,10-二氧代-1,4-亚蒽基)二亚氨基]双[(4-氯苯氧基)苯磺酸钠]
CAS：71720-84-8
分子式：C38H24Cl2N2O10S2·2Na
中文名称：[(9,10-二氢-9,10-二氧代-1,4-亚蒽基)二亚氨基]双[(4-氯苯氧基)苯磺酸钠]
英文名称：Benzenesulfonic acid, [(9,10-dihydro-9,10-dioxo-1,4-anthracenediyl)diimino]bis[(4-chlorophenoxy)-, disodium salt
分子式：C38H24Cl2N2O10S2·2Na
中文名称：[(9,10-二氢-9,10-二氧代-1,4-亚蒽基)二亚氨基]双[(4-氯苯氧基)苯磺酸钠]
英文名称：Benzenesulfonic acid, [(9,10-dihydro-9,10-dioxo-1,4-anthracenediyl)diimino]bis[(4-chlorophenoxy)-, disodium salt
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条