The physical rectangle scale includes the existing two-thirds endpoint buffer.
Equations
Instances For
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11GridPhysicalScale · compiled type and proof/definition references.
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11GridLong_rectangle · compiled type and proof/definition references.
The strict prefix and an occupied atom give the real physical x-window. It is not legal to replace x by N inside the distribution theorem.
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11GridPhysicalScale_window · compiled type and proof/definition references.
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11GridPhysicalScale_shift · compiled type and proof/definition references.
Before any later cell, the short distribution scale stays above a fixed power of N.
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11Grid_short_scale_lower · compiled type and proof/definition references.
The actual occupied two-dimensional grid has quadratic logarithmic cost.
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11GridUsed_card · compiled type and proof/definition references.
Any overhanging pair in an occupied rectangle remains below 4N.
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MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11Grid_pair_product_bound · compiled type and proof/definition references.