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Time-integrated and time-dependent angular analyses of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi><mml:mi>K</mml:mi><mml:mi>π</mml:mi></mml:math>: A measurement of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>cos</mml:mi><mml:mo></mml:mo><mml:mn>2</mml:mn><mml:mi>β</mml:mi></mml:math>with no sign ambiguity from strong phases

Time-integrated and time-dependent angular analyses of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>B</mml:mi><mml:mo>→</mml:mo><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi><mml:mi>K</mml:mi><mml:mi>π</mml:mi></mml:math>: A measurement of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>cos</mml:mi><mml:mo></mml:mo><mml:mn>2</mml:mn><mml:mi>β</mml:mi></mml:math>with no sign ambiguity from strong phases

We present results on $B\ensuremath{\rightarrow}J/\ensuremath{\psi}K\ensuremath{\pi}$ decays using ${e}^{+}{e}^{\ensuremath{-}}$annihilation data collected with the BABAR detector at the $\ensuremath{\Upsilon}(4S)$ resonance. The detector is located at the PEP-II asymmetric-energy storage ring facility at the Stanford Linear Accelerator Center. Using approximately $88\ifmmode\times\else\texttimes\fi{}{10}^{6}$ $B\overline{B}$ pairs, we measure the decay amplitudes for the flavor eigenmodes and …