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

  • Vertical lines: at the trivial zeros x = −2n (or shifted so that the critical line Re(s) = ½ is one edge).

  • Horizontal lines: at the non-trivial zero ordinates y = γₖ on Re(s) = ½.

The intersections form rectangular cells whose:

  • width = spacing of trivial zeros (W = 2),

  • 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:

  • Cell area: Aₖ = W * Δγₖ.

  • Triangle area: Aₖ^Δ = Δγₖ.

  • 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:

  • Cell scaling: Iₖ = Aₖ * log(γₖ / 2π) → 4π.

  • Triangle scaling: Jₖ = Aₖ^Δ * log(γₖ / 2π) → 2π.

  • 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:

  • Iₖ oscillates tightly around 4π with no drift.

  • Jₖ oscillates around 2π with no drift.

  • 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:

  • makes the density law immediately visible as shrinking cell height,

  • offers an intuitive “unity/duality” visual metaphor,

  • 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:

  • autocorrelation of the residuals Tₖ − π to test clustering,

  • extreme-value behavior of cell and triangle areas,

  • comparison with random-matrix models using the angle form,

  • 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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