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String Theory Demystified

String Theory Demystified

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CHAPTER 6<br />

BRST Quantization<br />

So far we have seen two methods that can be utilized to quantize the string: the<br />

covariant approach and light-cone quantization. Each offers its advantages.<br />

Covariant quantization makes Lorentz invariance manifest but allows for the<br />

existence of “ghost states” (states with negative norm) in the theory. In contrast,<br />

light-cone quantization is ghost free. However, Lorentz invariance is no longer<br />

obvious. Another trade-off is that the proof of the number of space-time dimensions<br />

(D = 26 for the bosonic theory) is rather diffi cult in covariant quantization, but it’s<br />

rather straightforward in light-cone quantization. Finally identifying the physical<br />

states is easier in the light-cone approach.<br />

Another method of quantization, that in some ways is a more advanced approach,<br />

is called BRST quantization. This approach takes a middle ground between the two<br />

methods outlined above. BRST quantization is manifestly Lorentz invariant, but<br />

includes ghost states in the theory. Despite this, BRST quantization makes it easier<br />

to identify the physical states of the theory and to extract the number of space-time<br />

dimensions relatively easily.<br />

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