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Transparencies pdf - Desy

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Consider first “small dipole - hadron” cross section<br />

d<br />

σinel = π2<br />

3 F2 d 2 αs(λ/d 2 )xGT(x.λ/d 2 )<br />

F 2 Casimir operator of color SU(3)<br />

F 2 F 2<br />

(quark) =4/3 (gluon)=3<br />

Comment: This simple picture is valid only in LO. NLO would require<br />

introducing mixing of different components. Also, in more accurate expression<br />

there is an integral over x, and and extra term due to quark exchanges<br />

26<br />

Baym et al 93<br />

26

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