偶宇称

O~（16）偶宇称态的结构（Ⅰ）

The structure of the even parity states of o ~ ( 16 ) ( I )

这些新测定的偶宇称能级属于4f~66s7S电子构型，位于33477～37758cm~（-1）能量范围。

These newly measured levels of even parity belong to 4 / 66s7S configuration and located in the energy range between 33477 and 37758 cm-1 .

Br2偶宇称里德堡态的转动结构和电子角动量

Rotational Structure and Electron Angular Momentum of the Gerade Rydberg State of Br_2

随着双阱势中势垒高度V0的不断增大，相邻的奇宇称能级与偶宇称能级逐渐接近，当V0→∞时，二者相等，能级由原来的非简并变成了简并。

The energy level of odd parity gradually approach that of even parity with increasing V_0.When V_0 approaches infinity , two energies are equal and the energy level changes from original non-degeneracy to degeneracy .

铈原子偶宇称自电离态激光共振电离光谱

Laser Resonance Ionization Spectroscopy of Even-Parity Autoionization States of Cerium Atom

采用一种与辐射传递方程偶宇称分解不同的处理方式推导了一个基于原始变量的二阶辐射传递方程。

A second order radiative transfer equation of primitive variable is derived by using a different way than the even parity formulation .

第三台染料激光波长在634～670nm范围内扫描，发现了141个偶宇称自电离态能级。

One hundred and forty-one autoionization states were found by these channels with the third-step laser scanning in the wavelength range of 634-670 nm .

该二阶方程具有辐射传递偶宇称公式的主要优点同时克服了其绝大部分缺点，可以方便的用于求解吸收、发射及各向异性散射介质内的辐射传递。

This second order equation possesses major advantages of the even parity formulation of radiative transfer , but overcomes most of its drawbacks , and can be conveniently applied to solve radiative transfer in absorbing , emitting and anisotropically scattering media .