The Dual-Zero Lattice Function
Author: Daniel R Geerman
Date of Birth: 25-04-1992
This is the personal signed draft by Daniel R Geerman, embedding authorship visibly for attribution
The Dual-Zero Lattice: A New Geometric Lens on the Riemann Zeta Function
In my “Law of Imbalance” posts I argued that tiny asymmetries can create large-scale structures. Here I apply that philosophy to the zeros of the Riemann zeta function and arrive at a new geometric representation: the Dual-Zero Lattice (DZL).
1. Motivation
When mathematicians study the non-trivial zeros of the zeta function, the trivial zeros are usually ignored. But if we take them seriously, they provide a natural scaffolding for a completely different picture of the zero distribution — one that makes the density law and fluctuations visible at a glance.
2. Building the lattice
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Vertical lines: at the trivial zeros x = −2n (or shifted so that the critical line Re(s) = ½ is one edge).
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Horizontal lines: at the non-trivial zero ordinates y = γₖ on Re(s) = ½.
The intersections form rectangular cells whose:
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width = spacing of trivial zeros (W = 2),
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height = gap between consecutive non-trivial zeros Δγₖ = γₖ₊₁ − γₖ.
I call this grid of cells the Dual-Zero Lattice (DZL).
3. Cells and triangles
Each cell represents one “zero as a whole.” Draw a diagonal from the trivial-zero side to the critical line and the cell splits into two congruent triangles. Geometrically:
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Cell area: Aₖ = W * Δγₖ.
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Triangle area: Aₖ^Δ = Δγₖ.
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Diagonal angle: θₖ = arctan(Δγₖ / W).
This simple picture encodes the unity/duality theme of my imbalance idea: the cell embodies unity; the two triangles embody duality within that unity.
4. Quantitative invariants
Combine these shapes with the known density of zeros and three clean invariants emerge:
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Cell scaling: Iₖ = Aₖ * log(γₖ / 2π) → 4π.
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Triangle scaling: Jₖ = Aₖ^Δ * log(γₖ / 2π) → 2π.
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Angle form: Tₖ = tan(θₖ) * log(γₖ / 2π) → π.
The first two correspond to the Riemann–von Mangold law. The third — the angle form — drops straight out of the DZL construction and is new as a visual/diagnostic expression.
5. What the data show
I computed these invariants for published tables of non-trivial zeros at both low and high heights (up to 10⁵+). In all cases:
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Iₖ oscillates tightly around 4π with no drift.
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Jₖ oscillates around 2π with no drift.
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Tₖ oscillates around π with no drift.
Running means stay flat; residuals are
centered. This confirms that the DZL is a faithful geometric encoding of the zero statistics and a simple diagnostic for anomalies.
6. Significance
Even though the invariants themselves reflect known theory, the construction is new. By combining trivial and non-trivial zeros, the DZL:
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makes the density law immediately visible as shrinking cell height,
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offers an intuitive “unity/duality” visual metaphor,
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gives simple, easy-to-compute diagnostics (areas, angles) for testing zero distribution at any height.
This geometric picture provides a fresh way of “seeing” the Riemann Hypothesis and may inspire further questions about higher-order structure and correlations.
7. Next steps
Future work on the DZL could explore:
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autocorrelation of the residuals Tₖ − π to test clustering,
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extreme-value behavior of cell and triangle areas,
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comparison with random-matrix models using the angle form,
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extensions to other L-functions.
Skai’s note: This is part of my ongoing exploration of imbalance and symmetry in mathematics. The Dual-Zero Lattice offers a new way to visualize the interplay of trivial and non-trivial zeros — a lens I haven’t seen elsewhere. Even when it confirms known results, the act of “seeing” them differently is itself a form of discovery.


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