Search for the $Z_1(4050)^+$ and $Z_2(4250)^+$ states in $\bar B^0 \to \chi_{c1} K^- \pi^+$ and $B^+ \to \chi_{c1} K^0_S \pi^+$

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The J / ψ {J\mskip-3.0mu/\mskip-2.0mu\psi\mskip 2.0mu} vertex position is used to define the three-momentum vector of the photon, and this is then added to the three-momentum of the associated e + e^{+} or e − e^{-} at this vertex. The electron mass is then assigned to this modified three-momentum vector, and the resulting four-momentum vector is used in calculating m ⁡ ( e + e − ) m(e^{+}e^{-})
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