Abstract
In preparation for a microscopic treatment of the low-energy, nucleus-nucleus optical potential, the static part of this potential (the pure one-channel problem) is reconsidered. Asymptotic nucleus-nucleus states are constructed via momentum-projection techniques of Rouhaninejad-Yoccoz type (1966) applied to localised fragment states, and are orthogonalised by diagonalising an overlap kernel. The relationship of the method to the resonating-group and complex-generator-coordinate methods and to the orthogonality-condition model is discussed in detail.
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