本征函数,eigenfunction
1)eigenfunction['aiɡ?n,f??k??n]本征函数
1.The tan~2x potential and the eigenvalue and eigenfunction for planar channelling radiation;正切平方势与平面沟道系统的本征值和本征函数
2.Green s Function of an Electrostatic Field Determined by Using Eigenfunction;用本征函数求静电场格林函数
3.A Sort of Novel Expression for the Eigenfunctions of Step Index Fiber;一种新的阶跃折射率光纤本征函数表达形式
英文短句/例句

1.Computation of Energy Levels of I_2 Molecule by Spherical Bessel Function Expansion MethodI_2分子振动本征函数的球贝塞尔函数展开法
2.The Stability of Bénard System and the Orthogonality of Eigenfunction;Bénard系统的稳定性与本征函数的正交性
3.EIGENFUNCTION METHOD FOR A GENERALIZATION OF BLACK-SCHOLES;推广的Black-scholes模型的本征函数解法
4.The parity of the eigenfunction is found by determining what happens to the wave function when r is replaced by -r.本征函数的宇称可以这样确定:当r用-r代替时看波函数的变化。
5.The value of the stationary states but also the corresponding functions ψ(orψ=ψe????), the so-called eigenfunctions.并且还给出相应的函数ψ(ψ=ψe????),这就是所谓的本征函数
6.Since we get continuous rather than discrete allowed values for E≥0, the positive-energy eigenfunctions are called continuum eigenfunction.由于对E≥0得到连续的而非分立的允许值,正能量的本征函数叫做连续谱本征函数
7.The procedure described above applies to the eigenvalues and eigenfunctions of any Hermitian operator.用上述运算方法也能求出任一厄密算符的本征值和本征函数
8.Quantum invariant eigenvalue and eigen function of quantum invariant operator of time-dependent damped harmonic oscilator;含时阻尼谐振子的量子不变量算符及其本征值和本征函数
9.Eigen-values and Eigen-wavefunctions of the Bound Electronic States in a Finite Semi-parabolic Quantum Well;有限深半抛物量子阱中束缚电子态的本征能量与本征函数
10.Calculation of energy characteristic value and characteristic function of hydrogen atoms with a kind of calculating signs;用一种算符计算氢原子的能量本征值和本征函数
11.It can always be arranged that degenerate eigenfunctions are orthogonal.总可以做到使得简并的本征函数是正交的。
12.If only the eigenvalue of A and not the eigenfunctions are desired, it is not necessary, according to Section 3. 3, to obtain the transformation matrix S.假如仅需求出A的本征值而不要求出本征函数,那么按照本章第3.3节,就不必求出变换矩阵S。
13.Since these eigenfunctions are equations we can graph them.由于这些本征函数是方程,所以我们能以图来描绘。
14.We always reject zero as an eigenfunction on the ground of physics.根据物理上的理由,我们总是剔除把零作为本征函数
15.In fact, we could make the substitution and still wind up with the correct eigenfunctions and eigenvalues.事实上,我们可以做这种代换而仍能绕弯得出正确的本征函数和本征值。
16.Dual Relation between Production Function and Cost Function;生产函数与成本函数的对偶关系及其特征
17.Wigner Functions for Eigenstates of Arbitrary Power of Annihilation Operators湮灭算符任意次幂本征态的Wigner函数
18.A research on intrinsic mode functions and the self-adjoint ordinary differential equations本征模式函数与自伴微分方程的关系研究
相关短句/例句

eigen function本征函数
1.The axial eigen functions of TE Z and TM Z modes with two layer or three layer dielectric radial waveguides were achieved by the boundary conditions on the basis of field distribution of eigen modes.首先根据平行板多层介质径向波导 (径向均匀 )本征模的场分布 ,讨论了两层和三层介质径向波导中TEZ模和TMZ 模的轴向本征函数 ,然后利用边界条件推导了相应的本征方程 ,最后探讨了本征方程的数值求解方法 ,同时对计算结果进行了分
2.So it is necessary to discuss the geometry meaning , eigen value, eigen function and character of projection operator in detail.因此 ,有必要详细地讨论投影算符的几何意义、本征值、本征函数及其性
3.The eigen functions {X\-n(x)} are orthogonal and an analytic solution is given at the end of this paper.通过提出一种变换 ,将两端系有不同集中质量的弹性杆的振动问题的边界条件化为第三类边条件 ,其本征值问题为规范的斯特姆 -刘维本征值问题 ,本征函数系 {Xn(x) }为正交完备的函数系 。
3)eigenfunctions本征函数
1.Symmetry of eigenfunctions on equilateral triangles正三角形上本征函数的对称性
2.In the finite square potential well a damped particle with a force quadratic in the velocity is studied,and thus it obtains the energy eigenvalues and energy eigenfunctions of the particle with a force quadratic in the velocity in infinitely deep square potential well.研究了方型势阱中的受到与速度平方成正比例的力的粒子 ,并得到了在无穷深势阱中受到与速度平方成正比例的力的粒子的能量本征值和能量本征函数
3.The eigenfunctions of some triangles with symmetric group,such as right angle isosceles,transform as one dimensional representation of this point group.几何上具有对称性的三角形,它的本征函数,也具有相应的对称性,即对称性群的一维表示。
4)eigenwave function本征波函数
5)intrinsic mode function本征模函数
1.The complicated original data set is decomposed into a series of intrinsic mode functions(IMF)and a residue by the empirical mode decomposition(EMD).此方法是通过经验模态分解(EMD)将一复杂的原始数据序列分解成一组本征模函数(IMF)和一个残余项,然后再对每一个IMF进行Hil bert变换。
6)eigenfunction method本征函数法
1.In this paper,eigenfunction method is used to calculate the coefficients of fractional parentage(CFP) of Fd 3 m  Fd 3 F 23 space group.利用陈金全教授的本征函数法计算了Fd 3m Fd 3 F 2 3空间群的母分系数 ,给出了求母分系数的计算步骤 ,并以实例来阐述求解过程 。
2.In this paper,eigenfunction method is used to calculate coefficients of fractional parentage(CFP) of Pn3mPn3P23 space group.本文利用陈金全教授的本征函数法计算了Pn3m Pn3 P2 3空间群的母分系数。
3.This paper introduces a method of deriving symmetrized wave function by eigenfunction method,using benzene C 6H 6 as an example.本文以苯分子C6H6为例 ,介绍了本征函数法求对称化波函数的一种方法 ,也就是把求群G的不可约表示基的问题转化为大家熟悉的求完备算符集共同本征函数问题 ,可以看出在此问题上 ,本征函数法较传统的群论方法要简
延伸阅读

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