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Transparencies pdf - Desy

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2 ! b P(b) / fm -1<br />

2 ! b P(b) / fm -1<br />

2<br />

1<br />

0<br />

0 1 2 3<br />

2<br />

1<br />

0<br />

b / fm<br />

P 2<br />

P 4<br />

P in<br />

s 1/2 =<br />

14000 GeV<br />

0 1 2 3<br />

b / fm<br />

P 2<br />

P 4<br />

P in<br />

s 1/2 =<br />

500 GeV<br />

2 ! b P(b) / fm -1<br />

2<br />

1<br />

0<br />

0 1 2 3<br />

b / fm<br />

P 2<br />

P 4<br />

P in<br />

s 1/2 =<br />

1800 GeV<br />

Difference between b-distributions for<br />

minimal bias and dijet, four jet events<br />

strongly increases with increase of incident<br />

energy. Solid lines: b–distributions for the<br />

dijet trigger, P2(b), with q⊥ = 25 GeV , as<br />

obtained from the dipole–type gluon<br />

ρ–profile. Long–dashed line: b–distribution<br />

for double dijet events, P4(b).<br />

Short–dashed line: b–distribution for<br />

generic inelastic collisions.<br />

40<br />

M.Strikman<br />

40

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