Literal (2.15) abscissa.
Equations
Instances For
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AnalyticNumberTheory.LargeSieve.panSourceSigma · compiled type and proof/definition references.
Literal (2.16) height.
Instances For
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AnalyticNumberTheory.LargeSieve.panSourceHeight · compiled type and proof/definition references.
Elementary telescoping majorant for the sum appearing in (2.23).
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AnalyticNumberTheory.LargeSieve.panHalfSum_le · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.panSourceSigma_bounds · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.panSourceSigma_power_le · compiled type and proof/definition references.
The original height dominates x^4 once log x ≥ 2; no change of T.
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AnalyticNumberTheory.LargeSieve.panSourceHeight_ge_fourth · compiled type and proof/definition references.
First displayed O-term in (2.23), with one absolute constant.
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AnalyticNumberTheory.LargeSieve.pan223_source_halfsum_bound · compiled type and proof/definition references.
Second displayed O-term of (2.23); y * sqrt y is y^(3/2).
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AnalyticNumberTheory.LargeSieve.pan223_source_sqrt_bound · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.pan_y_mul_sqrt · compiled type and proof/definition references.
Last O-term in (2.23). The hypothesis H ≤ x is explicit; this does not
claim to have substituted the later choice H=(2^j log^B x)^2.
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AnalyticNumberTheory.LargeSieve.pan223_source_inverse_square · compiled type and proof/definition references.
Literal y^(3/2) sqrt(H)/T rendering of the second bound.
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AnalyticNumberTheory.LargeSieve.pan223_source_three_halves_bound · compiled type and proof/definition references.
Equation (2.23), uniform eventual form. The absolute constant and threshold
precede q, the character, m, every cell, and the bounded coefficients.
The bound in fact does not need the source's extra restriction 1 ≤ A₁.
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AnalyticNumberTheory.LargeSieve.pan223_source_uniform_eventual · compiled type and proof/definition references.