本徵函數 的英文怎麼說

中文拼音 [běnzhǐhánshǔ]
本徵函數 英文
characdteristic function
  • 本 : i 名詞1 （草木的莖或根）stem or root of plants 2 （事物的根源）foundation; origin; basis 3 （本錢...
  • 徵 : 名詞[音樂] （古代五音之一 相當于簡譜的「5」） a note of the ancient chinese five tone scale corre...
  • 函 : 名詞1. [書面語] （匣; 封套） case; envelope 2. （信件） letter 3. （姓氏） a surname
  • 數 : 數副詞（屢次） frequently; repeatedly
  • 函數 : [數學] function函數計算機 function computer; 函數計算器 function calculator; 函數運算 functional operation
  1. Calculation of energy characteristic value and characteristic function of hydrogen atoms with a kind of calculating signs

    用一種算符計算氫原子的能量本徵值和本徵函數
  2. We always reject zero as an eigenfunction on the ground of physics.

    根據物理上的理由，我們總是剔除把零作為本徵函數。
  3. The parity of the eigenfunction is found by determining what happens to the wave function when r is replaced by －r.

    本徵函數的宇稱可以這樣確定：當r用r代替時看波函數的變化。
  4. The eigenvalue and eigenfunction of a coupled quantum oscillator

    二維耦合量子諧振子的本徵值和本徵函數
  5. The solutions of eigenvalue and eigenfunction for three non - self - adjont situation are summrized

    對三種非自共軛情形下的本徵值和本徵函數的求解方法進行了歸納總結。
  6. < uk > since we get continuous rather than discrete allowed values for e 0, the positive - energy eigenfunctions are called continuum eigenfunction. < / uk >

    < uk >由於對e 0得到連續的而非分立的允許值，正能量的本徵函數叫做連續譜本徵函數。 < / uk >
  7. 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.

    假如僅需求出A的本徵值而不要求出本徵函數，那麼按照本章第33節，就不必求出變換矩陣S。
  8. It can always be arranged that degenerate eigenfunctions are orthogonal.

    總可以做到使得簡並的本徵函數是正交的。
  9. The value of the stationary states but also the corresponding functions ψ(orψ=ψe), the so-called eigenfunctions.

    並且還給出相應的函數（e），這就是所謂的本徵函數。
  10. Since we get continuous rather than discrete allowed values for e≥0, the positive-energy eigenfunctions are called continuum eigenfunction.

    由於對E0得到連續的而非分立的允許值，正能量的本徵函數叫做連續譜本徵函數。
  11. The eigenfunctions of the gaudin differential / / - operators as the laughlin wavefunction are solved by bethe ansatz

    同時， gaudin模型l -運算元的本徵函數作為laughlin波函數也可以用betheansatz方法來求解。
  12. The governing equations of the problem are derived in hamiltonian form by using variable substitution and variational principle. then the methods of separation of variables and conjugate symplectic eigenfunction expansion are developed to solve the equations of plate bending problem. the result can be derived by analytical method

    在平面彈性問題中，由變量代換及變分原理，方程可導向哈密頓體系，從而通過分離變量法及共軛辛本徵函數向量展開法，以解析的方法來進行求解。
  13. Since these eigenfunctions are equations we can graph them.

    由於這些本徵函數是方程，所以我們能以圖來描繪。
  14. The procedure described above applies to the eigenvalues and eigenfunctions of any hermitian operator.

    用上述運算方法也能求出任一厄密算符的本徵值和本徵函數。
  15. In fact, we could make the substitution and still wind up with the correct eigenfunctions and eigenvalues.

    事實上，我們可以做這種代換而仍能繞彎得出正確的本徵函數和本徵值。
  16. We construct eigenfunctions from the linear combination of the b - spline functions and the truncated fourier series, and extend pseudospectral method to calculate above - threshold ionization electron spectrum of one - dimensional atom in intense laser fields. our results are also in very good agreement with those of split - operator method

    本文還利用b樣條函數和傅立葉級數的線性組合構造原子未微擾的本徵函數，將偽譜方法推廣用來計算一維模型原子在強激光場中的閾上電離譜，其結果與分裂算符方法所得的結果也符合得很好。
  17. This paper has studied the wavefunction expanded in terms of the two - dimensional harmonic oscillator eigenfunction through calculating the energy of the ground state, the energy of the first excited state and the oscillator strength in a square wire with finite barriers and studied its application in these fields. the most remarkable advantage of this wavefunction is that it can satisfy the continuity of the function and of its derivative divided by the band - mass and it is convenient to calculate some physical magnitudes because the number of the terms is small

    本文通過計算有限深方形量子線中單電子的基態能、第一激發態能和振子強度研究了以二維諧振子本徵函數為基展開的波函數以及它在這些問題中的應用，此波函數的顯著優點是：在邊界處滿足波函數的連續性條件和粒子流的守恆條件，並且展開項數少，計算方便。
  18. And beginning with a perturbed nls equation, using a multi - scales perturbation expansion, we get the zero order and the first order equations, discuss the eigenstates of the operator in the equations, induct relevant " derivative states ", form the completeness of the bounded eigenstates of the associated operator in li space, and expand the corresponding parameters in the closure, get a series evolution equations of the coefficients in the expanded formulas, find the first order approximate solution by researching the evolution equations. this paper also gives the basis of this method - the completeness we have formed and the singular perturbation technique

    ） dinser方程的求解問題，討論了自伴運算元的本徵函數的正交性和完備性，介紹了尋求微分方程的近似解常用的攝動方法，並從帶有某種擾動項的nls方程出發，利用多重尺度的攝動方法得到了方程的零級近似方程和一級近似方程，通過對近似方程中運算元的特徵態的討論，引入適當的「導出態」 ，建立了運算元在l _ 2空間的特徵態的完備性。
  19. In this paper, the wavefunction is expanded in terms of the two - dimensional harmonic oscillator eigenfunction and the mismatch of the effective mass is considered. we calculate the energy of the ground state, the energy of the first excited state and the oscillator strength of the single electron in a square quantum wire with finite barriers

    本文選取了以二維諧振子本徵函數為基展開的波函數，並且考慮了有效質量的失配性，計算了有限深方形量子線中單電子的基態能，激發態能和振子強度。
  20. The energy eigenvalue, eigenfunction, matrix elements of coordinate and momentum operators in energy representation, and evolution operator for a two - dimentional coupled oscillator are presented by using the general linear quantum transformation theory

    摘要運用廣義線性量子變換理論，給出一類二維耦合量子諧振子的能量本徵值、本徵函數、坐標和動量算符在能量表象中的矩陣元及演化算符。
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