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We present a search for a new narrow, spin-1, high mass resonance decaying to $\mu^+\mu^- + X $, using a matrix element based likelihood and a simultaneous measurement of the resonance mass and production rate.
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CDF uses a cylindrical coordinate system with the z z axis along the proton beam axis. Pseudorapidity is η ≡ − ln ( tan ( θ / 2 ) ) \eta\equiv-\ln(\tan(\theta/2)) , where θ \theta is the polar angle relative to the proton beam direction, and ϕ \phi is the azimuthal angle while p T = | p | sin θ p_{T}=|p|\ \sin\theta , E T = E sin θ E_{T}=E\ \sin\theta
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