| 1. | 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。 |
| 2. | 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。 |
| 3. | 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。 |
| 4. | 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。 |
| 5. | since we get continuous rather than discrete allowed values for e≥0, the positive-energy eigenfunctions are called continuum eigenfunction.
由于对E0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。 |
| 6. | 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33节，就不必求出变换矩阵S。 |
| 7. | The complete set of hydrogen atoms eigenfunctions in the momentum representation
动量表象中氢原子径向函数的完备集 |
| 8. | The eigenfunctions of the gaudin differential / / - operators as the laughlin wavefunction are solved by bethe ansatz
同时， gaudin模型l -算子的本征函数作为laughlin波函数也可以用betheansatz方法来求解。 |
| 9. | < 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。 < / uk > |
| 10. | 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 。 |
