Unit Shapes Distinguish Non-CM D6 Sextic Fields
Rank-2 log-unit lattices encode Galois structure and, for totally imaginary non-CM D6 sextics, determine the underlying field.
Underlying Paper
On the Geometry and Shapes of Rank 2 Log Unit Lattices
Every number field canonically gives rise to two lattices: its ring of integers and its log unit lattice. While the shapes of the former have undergone extensive research, far less is known about the shapes of the latter, referred to as unit shapes. This paper presents an in-depth analysis of the unit shapes of number fields with unit rank 2. Our first main result characterizes, in many cases, the location of unit shapes within the fundamental domain of the space of rank 2 lattice shapes in terms of the Galois group of the field's Galois closure, and determines when these unit shapes are transcendental. Next, we establish that the unit shape uniquely determines the field up to isomorphism for totally imaginary $D_6$ non-CM sextic fields; this result fails in the CM case. Finally, for certain subfamilies of $D_6$ non-CM imaginary sextics, we offer a simple sufficient condition for their log unit lattices to be orthogonal and provide lower bounds on the proportion of fields with orthogonal log unit lattice.
A number field has both an arithmetic lattice, its ring of integers, and a geometric object built from the logarithms of its units. The former has a substantial literature on lattice shapes; the latter has received much less systematic treatment. Cruz, Holmes, Jalalvand, Nunez Lon-Wo, Scheidler, and Tran study this second object for fields of unit rank 2, asking where its shape sits in the moduli space of rank-2 lattices and how much field-theoretic information the shape retains.
The paper's central point is that a log-unit lattice is not merely a coarse geometric invariant. In several rank-2 settings, its position in a fundamental domain reflects the Galois group of the Galois closure. For a particular family of imaginary sextic fields, the invariant is still stronger: the unit shape determines the field up to isomorphism, subject to an essential non-CM hypothesis.
Core Contribution
The authors organize rank-2 unit shapes through the standard fundamental domain for shapes of planar lattices. Rather than treating the regulator lattice only through its covolume, they retain its similarity class. This preserves angular information: an orthogonal log-unit lattice, for example, occupies a distinguished geometric position that cannot be recovered from the regulator alone.
Their first main result gives, in many cases, a characterization of where a unit shape lies in that domain in terms of the Galois group of the field's Galois closure. The paper also identifies cases in which the resulting shape is transcendental. This connects a geometric coordinate of a lattice-shape space to arithmetic symmetries of the field, rather than presenting shape as an unstructured numerical by-product of computing units.
For totally imaginary non-CM sextic fields, the authors prove an injectivity statement: equality of unit shapes forces isomorphism of fields. That claim is deliberately family-specific. The corresponding assertion fails in the CM case, so the result does not establish unit shape as a universal complete invariant for sextic fields.
Technical Approach
The construction begins with the log embedding of the unit group. After quotienting by torsion, a field of unit rank 2 supplies a rank-2 lattice in the relevant logarithmic hyperplane. Its shape is then represented in the fundamental domain for the action of on rank-2 lattice shapes. The analysis uses that representation to compare the geometry of a basis of logarithmic units with the arithmetic constraints imposed by the Galois closure.
The analysis separates non-CM and CM imaginary sextics. That separation is structural rather than cosmetic: the non-CM setting permits recovery of the field from the shape, while the CM setting supplies counterexamples to such recovery. The paper further isolates subfamilies of non-CM fields for which a simple sufficient condition makes the log-unit lattice orthogonal. This turns a geometric question about an angle into an arithmetic criterion that can be counted across a family.
Figure 1 displays unit shapes of signature sextics inside the fundamental domain. The plot makes the paper's use of shape concrete: the objects being classified are points or loci in a fixed moduli region, not only regulator values.
Results and Analysis
The strongest result is the uniqueness theorem for totally imaginary non-CM sextic fields. Within that stated family, the unit shape carries enough information to identify the isomorphism class. This is a sharper conclusion than locating a shape or distinguishing broad Galois behavior, but its scope matters: the authors explicitly report failure in the CM case.
The orthogonality results give the paper a second, population-level direction. For selected non-CM subfamilies, the authors provide a sufficient condition for orthogonal log-unit lattices and lower bounds on the proportion of fields satisfying it. The supplied material establishes the existence of those bounds but does not provide a numerical proportion here, so the result should be read as a rigorous family-specific counting statement rather than a broad empirical frequency claim.
This is theoretical evidence, not a benchmark study. Its value is the exact link between lattice geometry and field structure. For researchers working with regulators, unit groups, or arithmetic statistics of sextic fields, it offers a more discriminating invariant than covolume alone; for broader classes of number fields, the paper leaves open how often comparable rigidity survives.
Evidence Box
theoreticalKey Claims
- •Rank-2 unit-shape location reflects Galois-closure structure in many cases
- •Some rank-2 unit shapes are transcendental
- •Unit shape determines totally imaginary non-CM D6 sextic fields up to isomorphism
- •Arithmetic conditions can force orthogonal log-unit lattices in selected D6 families
Key Results
- •Rank-2 log-unit lattices are classified through the rank-2 lattice-shape fundamental domain
- •Totally imaginary non-CM D6 sextic fields are determined by their unit shape
- •The unit-shape uniqueness statement fails for CM D6 sextic fields
- •Lower bounds are established for orthogonal lattices in certain D6 non-CM sextic subfamilies
Limitations & Caveats
- •Analysis is restricted to fields of unit rank 2
- •Shape-based field recovery is proved only for totally imaginary non-CM D6 sextics
- •The corresponding uniqueness result fails in the CM D6 case
- •Orthogonality bounds apply only to selected D6 non-CM subfamilies