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We use 429 fb$^{-1}$ of $e^+e^-$ collision data collected at the $\Upsilon(4S)$ resonance with the BABAR detector to measure the radiative transition rate of $b\rightarrow s\gamma$ with a sum of 38 exclusive final states.
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Charge conjugation is implied throughout this study
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The Novosibirsk function is defined as f ( m E S ) = exp ( − 1 2 ( ln 2 [ 1 + Λ τ ( m E S − m ) ] / τ 2 + τ 2 ) ) f(m_{ES})=\mathrm{exp}\left(-\frac{1}{2}\left(\ln^{2}[1+\mathchar 28931\relax\tau(m_{ES}-m)]/\tau^{2}+\tau^{2}\right)\right) where Λ = sinh ( τ ln 4 ) / ( σ τ ln 4 ) \mathchar 28931\relax=\sinh(\tau\sqrt{\ln 4})/(\sigma\tau\sqrt{\ln 4}) , m m is the peak position, σ \sigma is the width, and τ \tau is the tail parameter
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