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In this article an experimental summary of the E(1420) meson with JPC=1⁺⁺ is presented and it is argued that the E(1420) is not explained by QCD in terms of being a fundamental arrangement of quarks and gluons. We then develop a final-state rescattering mechanism based on one-particle-exchange Born terms. We sum these Born terms through a Fredholm integral equation and obtain a Fredholm determinant which shows an enhancement at the E(1420) with JPC=1⁺⁺. The subsequent sum of Born terms is analogous to a {π} orbiting in a p wave around an s-wave KK{} system. This represents the first example of a molecular state which is bound by color-singlet particle exchanges, as opposed to work by Weinstein and Isgur, which uses color forces to bind their molecule. A phenomenological analysis of all the latest KK{}{π} data arising from hadroproduction argues that the molecular picture for the E(1420) is consistent. We show that if the molecular nature for the E(1420) is generated by the above final-state Born terms, an exotic K⁺K₀{K}⁺$ ${J}P$=${0}^{{{-}}}$ molecule must exist at the KK{}K threshold.
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R. S. Longacre (1990) studied this question.
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