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A mismatch penalty of 10kT would also give good recognition; however, obtaining that mismatch is challenging. If the penalty comes from a long range repulsive interaction, the two arrays will never come together. If the penalty comes from mismatched Watson-Crick pairing, then base flipping will never occur. If the penalty comes from a very short range interaction that does not require previous unbinding of a similar interaction, then the good recognition could be obtained, but we have not yet found a physically realizable system that embodies this requirement.
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A mismatch penalty of 10 k T would also give good recognition; however, obtaining that mismatch is challenging. If the penalty comes from a long range repulsive interaction, the two arrays will never come together. If the penalty comes from mismatched Watson-Crick pairing, then base flipping will never occur. If the penalty comes from a very short range interaction that does not require previous unbinding of a similar interaction, then the good recognition could be obtained, but we have not yet found a physically realizable system that embodies this requirement.
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Of course, if the sample is constrained so that the nearest available nonhomolog has m≠N sequence matches, then the energy gap between the two arrays can allow excellent homology stringency; however, in such a system the total number of distinguishable arrays would be limited by m regardless of the total length N of the arrays. More importantly, if the energy were linear then all of the binding sites would have to interact at once in correct registration in order to overcome the SSP. Those constraints actually represent the simple case where the N individual molecular contacts would be more correctly described as one single binding site that includes many molecular interactions.
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Of course, if the sample is constrained so that the nearest available nonhomolog has m ≠N sequence matches, then the energy gap between the two arrays can allow excellent homology stringency; however, in such a system the total number of distinguishable arrays would be limited by m regardless of the total length N of the arrays. More importantly, if the energy were linear then all of the binding sites would have to interact at once in correct registration in order to overcome the SSP. Those constraints actually represent the simple case where the N individual molecular contacts would be more correctly described as one single binding site that includes many molecular interactions.
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In contrast, in a system with a binding energy proportional to the number of bound triplets, adding more triplets would always be either favorable or unfavorable regardless of the number bound; therefore, either initial testing will be unfavorable, or the sequence independent binding would become increasingly deeply bound as more triplets were added, resulting in kinetic trapping.
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In contrast, in a system with a binding energy proportional to the number of bound triplets, adding more triplets would always be either favorable or unfavorable regardless of the number bound; therefore, either initial testing will be unfavorable, or the sequence independent binding would become increasingly deeply bound as more triplets were added, resulting in kinetic trapping.
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In vitro experiments featuring a single mismatched triplet followed by a series of matched triplets do show that skipping over a single triplet is not forbidden if subsequent regions contain substantial accidental homology.
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In vitro experiments featuring a single mismatched triplet followed by a series of matched triplets do show that skipping over a single triplet is not forbidden if subsequent regions contain substantial accidental homology.
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