From it is clear that D α (P, Q) has a steeper slope for increasing

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From it is clear that D α (P, Q) has a steeper slope for increasing
Inherent-state melting and the onset of glassy dynamics in two-dimensional supercooled liquids
From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
From it is clear that D α (P, Q) has a steeper slope for increasing
From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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From it is clear that D α (P, Q) has a steeper slope for increasing
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