Observation of the $\Upsilon(1^3D_J)$ Bottomonium State through Decays to $\pi^+\pi^-\Upsilon(1S)$

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Fermion-antifermion bound states are denoted n 2 S + 1 L J n^{2S+1}L_{J} , where n n , S S , L L , and J J are the radial, spin, orbital angular momentum, and total angular momentum quantum numbers of the pair
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