Finding the inverse of a large matrix often isn’t easy, so quantum physics calculations are sometimes limited to working with unitary operators, U, where the operator’s inverse is equal to its adjoint,
![image0.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe839_397744.image0.png)
(To find the adjoint of an operator, A, you find the transpose by interchanging the rows and columns, AT. Then take the complex conjugate,
![image1.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe833_397745.image1.png)
Note that the asterisk (*) symbol in the above equation means the complex conjugate. (A complex conjugate flips the sign connecting the real and imaginary parts of a complex number.)
This gives you the following equation:
![image2.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe82d_397746.image2.png)
The product of two unitary operators, U and V, is also unitary because
![image3.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe82a_397747.image3.png)
When you use unitary operators, kets and bras transform this way:
![image4.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe81a_397748.image4.png)
And you can transform other operators using unitary operators like this:
![image5.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe821_397749.image5.png)
Note that the preceding equations also mean the following:
![image6.png](https://cdn.prod.website-files.com/6634a8f8dd9b2a63c9e6be83/669d46b157331d6489bfe836_397750.image6.png)
Here are some properties of unitary transformations:
If an operator is Hermitian, then its unitary transformed version,
is also Hermitian.
The eigenvalues of A and its unitary transformed version,
are the same.
Commutators that are equal to complex numbers are unchanged by unitary transformations: