HIGHLIGHTS
SUMMARY
In terms of states with definite electric charge, Δ̂ and its VEV (vΔ ) are, respectively, Δ̂= p1ffiffi Δ̂- 2 Δ̂-- Δ̂0 - p1ffiffi2 Δ̂- 1 and hΔ̂i=pffiffiffi 2 vΔ In the pair and associated production_channels -LScalar=m2Δ̂ Tr½Δ̂† Δ̂ - λΔ1 (Tr½Δ̂† Δ̂ )2 - λΔ2 Tr½(Δ̂† Δ̂)2 † PHYS. Focusing first on the expected limits at small M Δ and small ΔM, one expects comparable signal contributions from the Δ-- Δ-- pair production process in Eq (22a) and the Δ Δ∓ associated production_channel in Eq (22b). As the mass splitting increases, two competing effects in the associate production_channel occur: (i) the Δ Δ∓ production cross section decreases due to . . .
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