13c-SiC中深杂质能级的A_1,T_2对称波函数 A_1, T_2 SYMMETRIC DEEP LEVEL wave functionS IN 3c-SiC 来源：学术文献
2由于波函数极值的空间距离而使得自发发射具有更低的概率，其直接效果是相对于具有I型接触的半导体系统延长了冷光衰变时间。 Due to the spatial distance of the wave function extremes, there is a lower probability of the spontaneous emission with the immediate consequence of an extended decay time of the luminescence relative to the semiconductor system with a type I contact. 来源：专利文献 中文专利号：CN101511601A 英文专利号：US2011006667
3在Glauber理论框架下，对13C（π+，π0）13N单电荷交换反应（Tx=150MeV和165MeV）进行分析，核波函数假定由价核子和12C核心组成，核心部分以独立a集团模型描述。 The SCX reaction 13C (π+,π0)13N at Tx = 150 MeV and 165 MeV are analyzed by using the frame of the Glauber theory. The nuclear wave function is assumed to be constructed by a vallence nucleon plus a core of 12C which is discribed by an independent a cluster model. 来源：学术文献
4然而，应当注意的是，第五比较实例的配置是这样的，折射率分布在通孔的直径方向即横向上逐渐变化，并且其基本构造概念与第一实施例的配置不同，在第一实施例中凸透镜作用使用交替设置层2A(交替设置层112A)产生，其结合了在具有大折射率的高折射率层21(高折射率层121)和具有小折射率的低折射率层20(低折射率层120)之间的光速不同的特征与波函数的连续性。 Note however, the arrangement of the fifth comparative example is such that a refractive index distribution is changed gradually in the diameter direction of the through hole, i.e., lateral direction, and the basic configuration concept thereof differs from that in the arrangement of the first embodiment wherein a convex lens effect is accepted using the alternate placement layer 2A (alternate placement layer 112A) which combines a feature wherein the velocity of light differs between the high refractive index layers 21 (high refractive index layers 121) having a great refractive index and the low refractive index layers 20 (low refractive index layers 120) having a small refractive index, and continuity of a wave function. 来源：专利文献 中文专利号：CN101320745A 英文专利号：US2009020690
5用屏蔽Coulomb近似波函数计算高Rydberg原子的l-混合跃迁截面 CALCULATION OF 1-MIXTURE TRANSITION CROSS ECTIONS OF HIGH RYDBERG ATOM BY USING SCREEN COULOMB APPROXIMATION wave functionS 来源：学术文献
1由于 E2跃迁算符 T(E2)q 是由群 U_(36),V_6(sd),SU_3(sd),SU_3(s)与 SU_3(s dS)的生成元构成的,故不必构造出强耦合 SU(3)极限的波函数,利用 Elliott 波函数妒φ((λμ)KJM)就可以得到 E2跃迁. The E2 transition operator T (E2)_q is composed of the generators of U(36),U_6(sd),(sd),SU_3(S)and SU_3(sdS),so the E2 transition can be obtained by using the Elliott wave-function Ψ((λ_μ)KJM)instead of calculating the wave-function of the strong coupling,SU(3)limit. 来源：学术文献
2π→eνγ过程和QCD中π介子波函数求和规则 π→eνγ Process and Pionic wave-function Sum Rule in QCD 来源：学术文献
3均匀弱电磁场中荷电空间转子的能级与波函数 Energy-Level and wave-function of the Charged Space Rotor in the Weak Uniform Electromagnetic Field 来源：学术文献
4取弱背景场A_u~3,由于耦合常数重整化与波函数重整化相关,计算仅需考虑A_μ~3的两点函数. 将所有有关的单圈图纳入计算过程后,得到了所需β参数的具体形式. As the coupling-constant renormalization is 'related to the wave-function renormalization, only the two-point function of the weak background A_μ~3 is considered. 来源：学术文献
5计算出该晶体的晶场参数,并由此得到了在晶场作用下4~F_(3/2),4~I_(11/2)和4~I_(9/2)三个谱项的所有斯塔克(Stark)子能级的本征波函数。 By using these parameters, the stark sub-level wave-functions of 4F3/2, 4I11/2 and 4I9/2 manifolds have been obtained. 来源：学术文献
