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Discover how polarizing beam splitters can be used for preparing and measuring polarized light.

We can express the square of the “length” of our quantum state vector in S=ahhlp+avvlp\ket S = a_\text{h} \ket{\text{hlp}} + a_\text{v} \ket{\text{vlp}} as follows:

 S 2=ah2+av2.\Vert~\vert S\rangle~\Vert^2 = a_{\text{h}}^2 + a_{\text{v}}^2.

I used quote marks around length for a state vector because that length is not something you can measure with a ruler. For almost all our work in quantum computing, we will use state vectors whose length is 11 (they are called “unit vectors” or “normalized vectors”). Following that convention, we will insist that

ah2+av2=1.a_{\text{h}}^2 + a_{\text{v}}^2 =1.

We will motivate that requirement in the next chapter.

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