Since these eigenfunctions are equations we can graph them . 由于這些本征函數(shù)是方程,所以我們能以圖來描繪。
It can always be arranged that degenerate eigenfunctions are orthogonal . 總可以做到使得簡并的本征函數(shù)是正交的。
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征值和本征函數(shù)。
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征函數(shù)和本征值。
since we get continuous rather than discrete allowed values for e≥0, the positive-energy eigenfunctions are called continuum eigenfunction. 由于對E0得到連續(xù)的而非分立的允許值,正能量的本征函數(shù)叫做連續(xù)譜本征函數(shù)。
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的本征值而不要求出本征函數(shù),那么按照本章第33節(jié),就不必求出變換矩陣S。
The complete set of hydrogen atoms eigenfunctions in the momentum representation 動量表象中氫原子徑向函數(shù)的完備集
The eigenfunctions of the gaudin differential / / - operators as the laughlin wavefunction are solved by bethe ansatz 同時, gaudin模型l -算子的本征函數(shù)作為laughlin波函數(shù)也可以用betheansatz方法來求解。
< uk > since we get continuous rather than discrete allowed values for e 0 , the positive - energy eigenfunctions are called continuum eigenfunction . < / uk > < uk >由于對e 0得到連續(xù)的而非分立的允許值,正能量的本征函數(shù)叫做連續(xù)譜本征函數(shù)。 < / uk >
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的本征值而不要求出本征函數(shù),那么按照本章第3 3節(jié),就不必求出變換矩陣s 。