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nondegenerate     
相关语句
  非退化
     Let X(t)=X(0)+∫\+t\-0α(X(s)) d B(s)+∫\+t\-0β(X(s)) d s be a d dimensional nondegenerate diffusion process, where B(t) is a Brownian motion.
     设 X(t) =X(0 ) +∫t0 α(X(s) ) d B(s) +∫t0 β(X(s) ) ds为一 d(d≥ 3)维非退化扩散过程 .
短句来源
     Suppose that (λ0,u0) is a nondegenerate turning point of the Navier-Stokes equations.
     设(λ0,u0)是Navier-Stokes方程的非退化转向点,其中λ0=1/Re0。 Re0为雷诺数.
短句来源
     (2) Let Mn(n≥2) be a nondegenerate affine hypersurfacein An+1,then K is covarant-Symmetric if and only if M is an affine hypersphere;
     (2)若Mn(n≥2)是An+1中非退化的仿射起曲面,则K共变对称当且仅当M是仿射球;
短句来源
     With the method of Moving Frames this paper has proved: If Mn (n ≥2) is a nondegenerate affine hypersurface in An+1, (1) Suppose ■K = 0 (The difference tensor K is parallel), then M is an affine hypersphere with J = 0 and G is an Einstein's affine metric, Here J is Pick invariant of M and G is the Blaschke metric.
     本文用活动标架法证明了:若 Mn(n≥2)是 n+1维仿射空间 An+1中非退化的仿射超曲面,(1)若■K=0(即差异张量平行),则M是仿射球,且J=0和G是一个Einstein度量,这里J是M的 Pick不变量,G是Blaschke度量;
短句来源
     The Boundary Behaviour of Integral Representation on the Real Nondegenerate Weil Polyhedron on Stein Manifolds
     Stein流形上实非退化Wed多面体积分表示的边界性质
短句来源
更多       
  非简并
     STUDY ON THE NONDEGENERATE FOUR-WAVE MIXING OF Eu∶ Fe∶LiNbO3 CRYSTAL
     Eu∶Fe∶LiNbO_3晶体非简并四波混频的研究
短句来源
     Application of SU(2)canonical transformation and pseudo vector model in the nondegenerate two photon jaynes cumming model
     SU(2)正则变换及赝矢量模型在非简并双光子Jaynes-Cummings模型中的应用
短句来源
     Nondegenerate four-wave mixing in proton exchanged LibNO_3 planar optical waveguide
     质子交换LiNbO_3平面光波导中的非简并四波混频
短句来源
     Using He-Ne laser of 632.8nm as the signal beam and a pump beam, using Ar+ laser of488.0nm as the another pump beam,the nondegenerate four-wave mixing was realized in the Eu∶ Fe∶LiNbO3 crystal. The frequency-varied phase conjugation beam of 488.0nm was obtaind. At the sametime,a same-freguency conjugation beam of 632.8nm was obtained as well.
     用波长为623.8nm的He-Ne激光作信号光和一束泵浦光,用波长为488.0nm的Ar+激光作另一束泵浦光,在Eu∶Fe∶LiNbO_3晶体中实现了非简并四波混频,获得了波长为488.0nm的变频相位共轭光,同时还产生了波长为632.8nm的同频相位共扼光。
短句来源
     Theoretical analysis of highly nondegenerate Four-Wave Mixing in DFB laser
     DFB半导体激光器的非简并四波混频理论分析
短句来源
更多       
  非退化
     Let X(t)=X(0)+∫\+t\-0α(X(s)) d B(s)+∫\+t\-0β(X(s)) d s be a d dimensional nondegenerate diffusion process, where B(t) is a Brownian motion.
     设 X(t) =X(0 ) +∫t0 α(X(s) ) d B(s) +∫t0 β(X(s) ) ds为一 d(d≥ 3)维非退化扩散过程 .
短句来源
     Suppose that (λ0,u0) is a nondegenerate turning point of the Navier-Stokes equations.
     设(λ0,u0)是Navier-Stokes方程的非退化转向点,其中λ0=1/Re0。 Re0为雷诺数.
短句来源
     (2) Let Mn(n≥2) be a nondegenerate affine hypersurfacein An+1,then K is covarant-Symmetric if and only if M is an affine hypersphere;
     (2)若Mn(n≥2)是An+1中非退化的仿射起曲面,则K共变对称当且仅当M是仿射球;
短句来源
     With the method of Moving Frames this paper has proved: If Mn (n ≥2) is a nondegenerate affine hypersurface in An+1, (1) Suppose ■K = 0 (The difference tensor K is parallel), then M is an affine hypersphere with J = 0 and G is an Einstein's affine metric, Here J is Pick invariant of M and G is the Blaschke metric.
     本文用活动标架法证明了:若 Mn(n≥2)是 n+1维仿射空间 An+1中非退化的仿射超曲面,(1)若■K=0(即差异张量平行),则M是仿射球,且J=0和G是一个Einstein度量,这里J是M的 Pick不变量,G是Blaschke度量;
短句来源
     The Boundary Behaviour of Integral Representation on the Real Nondegenerate Weil Polyhedron on Stein Manifolds
     Stein流形上实非退化Wed多面体积分表示的边界性质
短句来源
更多       
  “nondegenerate”译为未确定词的双语例句
     Effects of self-phase modulation on the cavity field spectra of the nondegenerate two-photon J-C model
     相位自调制效应对两模双光子J-C模型腔场谱的影响
短句来源
     Furthermore,we discussed the Hausdorff dimension and Packing dimension of inverse image and level sets of N-dimension nondegenerate diffusion processes.
     lder连续性和扩散过程样本逆象集与水平集的 Hausdorff维数和Packing维数 .
短句来源
     Tunable range is 40nm. Mixing the output of SFRL with SDH optical signal in SOA,Highly nondegenerate FWM is demonstrated. Results for -19.49nm,down and 7.04nm up wavelength conversion with input signal at 2.5Gb/s have been obtained.
     优化设计半导体光纤环形激光器 (SFRL)产生波长连续可调谐窄线宽的激光输出 ,可调谐范围为 40 nm,利用半导体光放大器 (SOA)的非线性效应四波混频 (FWM) ,实现了码速为 2 .5 Gb/ s SDH信号光的波长变换 ,向上变换 7.0 7nm,向下变换 1 9.49nm.
短句来源
     The cavity field spectra for the nondegenerate two-photon Jayners-Cummings model with an additional Kerr-like medium were investigated.
     研究了充满Kerr介质的高Q腔中二能级原子和双光子Jaynes-Cummings模型腔场谱。
短句来源
     We have studied the influence of the Kerr effect on the average photon numbers, the degrees of second-order coherence, the degree of interbeam second-order coherence and the Cauchy-Schwartz inequality in the system consisting of an nondegenerate two-photon J-C model in a high-Q cavity filled with a Kerr-like medium.
     研究了一位于高Q Kerr介质腔中的二能级原子与双模光场相互作用系统中,Kerr效应对光场单模平均光子数、单模二阶相干度、两模间的相关性,以及Cauchy-Schwartz不等式的影响。
短句来源
更多       
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  nondegenerate
The space itself can be characterized essentially as the domain where the generalized Bergman operator is nondegenerate.
      
The present paper contains a systematic study of the structure of metric Lie algebras, i.e., finite-dimensional real Lie algebras equipped with a nondegenerate invariant
      
The Brockett problem for second-order systems with scalar feedback and nondegenerate transfer function is shown to have a positive solution.
      
Solution was determined in a general form, and the existence theorem was proved for the nondegenerate case.
      
A finite-dimensional nondegenerate system of algebro-differential equations with discontinuances is considered.
      
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By a new choice of the vacuum state it is shown that the nondegenerate Brueckner-Goldstone linked cluster expansion formula can also be applied to the case where there is one particle outside or one hole inside the closed shell configuration, even though here exists degeneracy.

本文的目的是指明,倘满壳层外只有一个粒子或只含一个空穴,即使情态存有退化,我们仍可以求得消去了所有含有粒子自能图的项、而且在形式上和满壳层情况完全一样的相连项展开公式。

In this paper the nondegenerate modes in multi-element PCR have been derived by means of the first form[1,2] and the second form[3,4] of transfer matrices for the PCM.

本文应用PCM变换矩阵的两种形式计算了非简并情况下多元件PCR腔镜上的模,得出了稳定条件和模的微扰稳定性质。

Using the method of transient capacitance at constant temperature, the shift of gold acceptor energy level in silicon under 〈100〉 , 〈110〉 , 〈 111〉 uniaxial press has been studied. Considering the split of conduction band caused by uniaxial stress, a formula for electron emission rate from deep center to conduction band has been derived. With this formula and experimental data of emission rate and reported tangential deformation potential constant Eu ,the active energy of gold acceptor under various uniaxial...

Using the method of transient capacitance at constant temperature, the shift of gold acceptor energy level in silicon under 〈100〉 , 〈110〉 , 〈 111〉 uniaxial press has been studied. Considering the split of conduction band caused by uniaxial stress, a formula for electron emission rate from deep center to conduction band has been derived. With this formula and experimental data of emission rate and reported tangential deformation potential constant Eu ,the active energy of gold acceptor under various uniaxial stress has been determined. In the range of experimental stress (0-9 kbar), a linear dependence of active energy on stress has been found. When uniaxial presses are parallel to 〈110〉 ,〈111〉 crystal orientations, the proportionality constants are α〈110〉 = -3.2±0.6 meV/kbar, α〈111〉 =-0.3±0.6 meV/kbar respectively. When uniaxial press is parallel to 〈100〉 crystal orientation and if we take Eu = 9.2 eV, 〈100 〉= -5.8± 0.8 meV/kbar, or if Eu =11.4 eV, α〈100〉 =-5.3± 0.8 meV/kbar. The changes of active energy are strongly anis-otropic. Further more, we have determined the shift coefficients of gold acceptor level in the presence of uniaxial stress relative to the bottom of conduction band in the absence of uniaxial stress. When Eu =9.2 eV, the coefficients are S〈100〉=-1.3±0.8 meV/kbar, S 〈110 〉=0.7±0.6 meV/kbar, S〈111〉=-0.7±0.6 meV/kbar respectively, when Eu =11.4 eV, the values are S〈100〉 = - 3.5± 0.8 meV/kbar, S〈110〉 = 0.0 ±0.6 meV/kbar, S〈111〉=- 1.0 ± 0.6 meV/kbar. Deviations among three coefficients of each group are larger than uncertainty of experiments. Thus, the possibility that gold centers in silicon have cubic symmetry and at the same time both negatively charged and neutral gold centers have nondegenerate basic states is quite small.

用恒定温度下瞬态电容法研究了硅中金受主能级在沿〈100〉,〈110〉,〈111〉晶向单轴应力作用下的能级移动。考虑到硅的导带在单轴应力下的分裂,导出了单轴应力下深中心中电子发射率的公式。根据该式和发射率的实验数据以及切变畸变势常数,求出了金受主能级激活能随应力的改变。在实验应力范围内(0—9kbar),激活能与应力成线性关系。当应力平行于〈110〉〈111〉晶向时,激活能随应力改变的斜率分别为α_(<110>)=-3.2±0.6meV/kbar,α_(<111>)=-0.3±0.6meV/kbar;当应力平行于〈100〉晶向,若取Ξ_u=9.2eV,α_(<100>)=-5.8±0.8meV/kbar,若取Ξ_=11.4eV,α_(<100>)=-5.3±0.8meV/kbar,α表现出强烈的各向异性。进一步确定了金受主能级相对于零压力下导带底的绝对移动的压力系数。若取Ξ_u=9.2eV,这些系数分别为S_(<100>)=-1.3±0.8meV/kbar,S_(<110>)=0.7±0.6meV/kbar,S_(<111>)=-0.7±0.6meV/kbar。如取Ξ=11.4eV,则S_(<100>)=-3....

用恒定温度下瞬态电容法研究了硅中金受主能级在沿〈100〉,〈110〉,〈111〉晶向单轴应力作用下的能级移动。考虑到硅的导带在单轴应力下的分裂,导出了单轴应力下深中心中电子发射率的公式。根据该式和发射率的实验数据以及切变畸变势常数,求出了金受主能级激活能随应力的改变。在实验应力范围内(0—9kbar),激活能与应力成线性关系。当应力平行于〈110〉〈111〉晶向时,激活能随应力改变的斜率分别为α_(<110>)=-3.2±0.6meV/kbar,α_(<111>)=-0.3±0.6meV/kbar;当应力平行于〈100〉晶向,若取Ξ_u=9.2eV,α_(<100>)=-5.8±0.8meV/kbar,若取Ξ_=11.4eV,α_(<100>)=-5.3±0.8meV/kbar,α表现出强烈的各向异性。进一步确定了金受主能级相对于零压力下导带底的绝对移动的压力系数。若取Ξ_u=9.2eV,这些系数分别为S_(<100>)=-1.3±0.8meV/kbar,S_(<110>)=0.7±0.6meV/kbar,S_(<111>)=-0.7±0.6meV/kbar。如取Ξ=11.4eV,则S_(<100>)=-3.5±0.8meV/kbar,S_(<110>)=0.0±0.6meV/kbar,S_(<111>)=-1.0±0.6meV/kbar。同一组的三个绝对移动值之间的偏离都超过了实验误差这一事实,说明了金中心具有立方对称性,同时中性金与带负电的金的基态都是非简并的可能性很小。

 
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