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note
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The explanation of the dynamics given here by the present authors is slightly different from the discussion by Ediger and coworkers [6,7] in which they assumed a large molecular mobility in the top few nanometers of the glass during deposition. The present authors consider in contrast that the dynamic interaction responsible to the formation of the dense glass may be restricted in a small range within a few molecules around a deposited molecule. This is related to the anomalous intermolecular conformation described in the last part of the paper.
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