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SUSY Dark Matter and Colliders - whepp-9

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Funnel Accuracies<br />

SM inputs <strong>and</strong> tan β uncertainties can be controlled<br />

by measuring M A , Γ A . Aχ 0 1χ 0 1 coupling ∼ 1/µ.<br />

Γ A ∝ M A tan 2 β(m 2 b + m2 τ) (γγ option of LC,<br />

A → µµ at LHC).<br />

a<br />

10<br />

1<br />

0.1<br />

0.01<br />

0.001<br />

M 1/2<br />

-<br />

m t<br />

α s (M Z )<br />

m b<br />

m 0<br />

∆A 0<br />

tanβ<br />

0<br />

50 100 150 200 250 300 350 400 450 500<br />

m 0 χ1<br />

(GeV)<br />

200<br />

150<br />

100<br />

50<br />

∆A 0 (GeV)<br />

a<br />

100<br />

10<br />

1<br />

0.1<br />

0.01<br />

a(Γ A )<br />

a(M χ1<br />

0)<br />

a(M A )<br />

a(2M χ1<br />

0 - M A )<br />

a(µ)<br />

2M χ1<br />

0 - M A<br />

-20<br />

-40<br />

-60<br />

-80<br />

-100<br />

-120<br />

50 100 150 200 250 300 350 400 450 500<br />

M 0 χ1<br />

(GeV)<br />

0<br />

2M χ1<br />

0 - M A (GeV)<br />

<strong>SUSY</strong> <strong>Dark</strong> <strong>Matter</strong> <strong>and</strong> <strong>Colliders</strong><br />

B.C. Allanach – p.37/53

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