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We present a search for a new heavy particle $M$ produced in association with a top quark, $p\bar{p}\rightarrow t(M \rightarrow \bar{t}q)$ or $p\bar{p}\rightarrow \bar{t}(\bar{M}\rightarrow t\bar{q})$, where $q$ stands for up quarks and down quarks.
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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
Cited in the paper.
Missing transverse momentum, E T {\not\!\!E_{T}} , is defined as the magnitude of the vector − ∑ i E T i n → i -\sum_{i}E_{T}^{i}\vec{n}_{i} where E T i E_{T}^{i} are the magnitudes of transverse energy contained in each calorimeter tower i i , and n → i \vec{n}_{i} is the unit vector from the interaction vertex to the tower in the transverse ( x , y x,y ) plane
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This region simultaneously satisfies the observed high- m t t ¯ m_{t\bar{t}} A f b A_{fb} , low- m t t ¯ m_{t\bar{t}} A f b A_{fb} , and the t t ¯ t\bar{t} cross-section better than the standard model. Mathematically, it is defined as the region with χ 2 < 2.8 \chi^{2}<2.8 , where χ 2 \chi^{2} is defined in Equation 22 in Ref. [ 4 ] . χ 2 \chi^{2} for the standard model is 2.8
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