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If none of the modes: (formula presented), and, enter the channel, the condition in Eq. (21) does not have to be fulfilled for these modes. For a hard-wall potential of width, one can prove: (formula presented)
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If none of the modes: (formula presented) m, and n enter the channel, the condition in Eq. (21) does not have to be fulfilled for these modes. For a hard-wall potential of width d one can prove: (formula presented)
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