| 1. | We can not say for certain which eigenvalue will be obtained .
我们不能说一定得到哪个本征值。 |
| 2. | Notice that the energy eigenvalues are not equally spaced .
注意，这些本征值并不是等距离分布的。 |
| 3. | 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。 |
| 4. | 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。 |
| 5. | To this end we shall first consider the following eigenvalue problem .
为此目的，我们将首先考虑下列的本征值问题。 |
| 6. | 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。 |
| 7. | For longer wavelengths a number of extrinsic photoconductive devices exist .
对于更长的波长，有许多非本征光电导器件可用。 |
| 8. | Determine the most probable position(s)of the electron for each eigenstate .
试对各个本征态，分别确定电子最可能出现的一个（或几个）位置。 |
| 9. | the roots of the characteristic equations are known as eigenvalues, or characteristic values.
特征方程之根称为本征值或特征值。 |
| 10. | 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。 |
