Categories · Algebra · Geometry · Logic
A mathematical object is rarely given by one single "true" description. Real numbers, Boolean algebras, graphs — all of them live in several theories at once. An object's true nature is an invariant: whatever survives the passage from one language to another. But the passages themselves come in very different strengths and shapes. Below we build a "periodic table" of such translations, work out a basic method for using them, and look at some classical examples.
Any translation between mathematical theories is characterized by two main coordinates: information preservation (rows 1, 2, 3) and the direction of the arrows (columns A, B). Inside every cell a third dimension appears (I, II, III) — namely, exactly what we work with: formalism (equations, axioms) or semantics (spaces, the object's reality).
| A. Covariant Translation (Order is preserved) |
B. Contravariant Translation (Order is reversed) |
|
|---|---|---|
| 1. Strict Reversibility (Bijection / Isomorphism) |
1A
Equivalences
|
1B
Strict Dualities
|
| 2. Embedding and Approximation (Injection / Galois connection) |
2A
Embeddings and Representations
|
2B
Galois Connections
|
| 3. Compression (Projection / Invariant) |
3A
Covariant Invariants
|
3B
Contravariant Invariants
|
Determines whether we lose data along the way. Row 1 is a bijection: absolutely everything translates, nothing is lost. Row 2 is an injection or a closure: we embed the object into a wider context (where extra, untranslatable structure appears) or find its best approximation. Row 3 is a projection (compression): information is irreversibly lost, we discard detail and keep only the "core" (the invariant).
Column A (Covariance): structure maps to structure, subset to subset, order is preserved. Column B (Contravariance): the single most interesting property in mathematics. Order is reversed: a substructure on one side corresponds to a quotient structure (or an orthogonal complement) on the other. Big becomes small.
An axis running through all of mathematics, from logic to algebraic geometry. Formalism (syntax) is formulas, equations, axioms, ideals of polynomials — the language itself. Semantics (ontology) is models, spaces, varieties of roots, concrete algebras — the reality standing behind the language. The most powerful theorems (Hilbert's Nullstellensatz, for instance) are translations of type III (Formalism ↔ Semantics).
Throughout this table we assume the translation is canonical (natural, independent of any choice we make). If non-canonical translations are allowed — ones requiring a choice of basis, or the Axiom of Choice — "exotic" cells appear. For instance, the isomorphism \(V \cong V^*\) for finite-dimensional spaces, or the field isomorphism \(\mathbb C \cong \mathbb C_p\). Such translations exist abstractly, but break under a change of basis and are useless for carrying computations through.
Any coordinate from the table above is used to carry problems between theories. The working scheme has four steps:
This four-step scheme is an ideal. Its weak point is step 4 (back-translation). For it to work, language \(\mathcal D\) must not forget what was said in language \(\mathcal C\). For the first three kinds of translation (row 1: bijections, equivalences, dualities) reversibility is guaranteed, and the scheme works flawlessly. But losses grow as we move down the list: embedding into a specific class (row 2) introduces untranslatable "extra" structure, and at the level of invariants (row 3) step 4 disappears completely — once the structure has been discarded, there is no going back.
Below is a survey of classical mathematical results, each tagged with its exact coordinates in the Periodic Table.
Objects of different nature turn out to be one and the same object (isomorphism), or a single structure is given by two vocabularies at once (definitional equivalence).
We stay within the text of the axioms, but reverse the order. Every true statement rewrites into its dual.
Polarity with respect to the conic itself sends a point \(P\) on the conic to the tangent \(t_P\) at that point, and sends the conic to itself. So the inscribed hexagon turns into the circumscribed one, the side \(P_iP_{i+1}\) turns into the vertex \(Q_i=t_i\cap t_{i+1}\), the intersection point of opposite sides turns into the diagonal joining opposite vertices, and "three points are collinear" turns into "three lines are concurrent."
The same polarity works one dimension up — no longer with respect to a conic in the plane, but with respect to the sphere itself. On the unit sphere \(S^2\subset\mathbb R^3\), the role of "lines" is played by great circles — the sections of the sphere by planes through its center.
Just as with the conic, this polarity carries an entire figure to its dual. Take a spherical triangle \(ABC\) (sides are arcs of great circles) and its polar triangle \(A^{*}B^{*}C^{*}\), where \(A^{*}\) is the pole of side \(a=BC\), and so on. The pole of a side of the original triangle turns out to be a vertex of the dual one — exactly the same "side ↔ vertex" transformation as with Pascal and Brianchon.
If you drag all three points onto almost a single great circle (the limiting, degenerate configuration), the polar triangle on the right may start looking jagged, and its perimeter and angles can jump sharply from frame to frame. That's not a bug — it's a genuine instability of the polarity itself at that point: a side's pole is chosen between two antipodal points on the sphere by the sign of a dot product with the third vertex, and near degeneracy that vertex ends up almost exactly on the boundary between "plus" and "minus" — the slightest shift can flip the pole to the opposite side of the sphere. How strongly and abruptly this shows up depends precisely on how evenly (or not) the three points are spread along that limiting circle.
Polarity translates not only figure to figure, but measure to measure. Here it is important not to confuse the point \(A\) (a vertex, an element of the sphere) with the angle at vertex \(A\) — the dihedral angle between sides \(b\) and \(c\) meeting at that point; denote it \(\angle A\). Likewise, don't confuse the side-arc \(a=BC\) (a set of points) with its length — also denoted \(a\) by tradition: \(a=|BC|\), the length of the great-circle arc from \(B\) to \(C\), which on the unit sphere (radius \(1\)) coincides with the central angle \(\angle(OB,OC)\) in radians. Likewise \(a^{*}=|B^{*}C^{*}|\) — the length of a side of the polar triangle, a number, not the arc itself. A classical fact of spherical trigonometry: a side of the polar triangle supplements to \(\pi\) the opposite angle of the original, and conversely — \(a^{*}=\pi-\angle A\), \(\angle A^{*}=\pi-a\) (and likewise for the other pairs). Where polarity for the conic swapped "side" and "vertex" of a polygon, here it swaps "side" (arc length) and "angle" — that is its metric face.
If antipodal points are identified (\(P\) and \(-P\) counted as one point), great circles become "lines" for which all the axioms of absolute geometry hold except one: any two lines meet, in exactly one point — there are no parallels. This is elliptic geometry, the third classical constant-curvature geometry alongside Euclidean (zero curvature) and hyperbolic/Lobachevskian geometry (negative curvature); the sphere with antipodes identified (\(\mathbb{RP}^2\) with its metric) is its standard model.
On the sphere itself, without identification, there is a small subtlety: two great circles meet not in one but in two (antipodal) points, and through a pair of antipodes there passes not a single line but a whole pencil of them. This version is sometimes called "double elliptic geometry." It has no effect on the point↔circle duality itself: a circle has exactly two poles, but they are antipodal and define the very same polar circle — so for the purposes of polarity it makes no difference whether one works on the sphere itself or after identification.
The highest art of translation. Structures of different nature are linked functorially, with an exact reversal of order.
Formalism embeds into formalism, preserving derivability, but without any way of strictly returning to the original.
The abstract is realized concretely. The translation carries information into a more tangible medium, but adds "scaffolding" to the object (a basis, coordinates, the specifics of a set).
Words become objects. We take formalism and turn it into a semantic object.
Antitone translations on a single ontological level.
The same antitonicity as above, but now between syntax and semantics.
Information loss as a working method. The assignment is not reversible, but what gets discarded does not get in the way of computation.
Compressing formalism into a mathematical measuring object.
It sounds paradoxical (we compress information, yet the arrows reverse), but behind it lies a geometric idea: observation through functions.
The most powerful tools in engineering and mathematics work because they punch through several cells of our table at once.
Why are generating functions, Fourier series, and the Laplace transform so effective? In all of these translations the invariant core is the same: convolution turns into pointwise multiplication, and differentiation turns into multiplication by the variable. A differential equation becomes algebraic, is solved by division, and back-translation (Step 4) returns the answer.
This trick is a layer cake of three translations from the Periodic Table:
A summary of the hypotheses most often dropped from statements. Each row is a place where the translation stops working once the condition is lifted.
| Tool | Required Hypothesis | What Happens Without It |
|---|---|---|
| Stone's theorem | The Boolean prime ideal theorem \(\mathsf{BPI}\) | In \(\mathsf{ZF}\) without \(\mathsf{BPI}\) there may not be enough ultrafilters. \(\mathsf{BPI}\) is strictly weaker than \(\mathsf{AC}\). |
| The Galois correspondence | Finiteness + normality + separability | Infinite extensions need the Krull topology, and the correspondence works only for closed subgroups. |
| The duality principle | Self-duality of the axiom list | In intuitionistic logic \(\neg\neg x\ne x\), and the symmetry collapses. |
| Gelfand, the non-unital case | Proper continuous maps | An arbitrary continuous map \(X\to Y\) does not induce a homomorphism the other way — the correspondence breaks. |
| Categoricity of \(\mathbb R\) | The second-order completeness axiom | The first-order theory of real closed fields is not categorical (Löwenheim–Skolem): non-standard non-Archimedean models appear. |
| Bi-interpretability | Reversibility of the translations | \(\mathsf{ZF}\) and \(\mathsf{ZFC}\) are mutually interpretable, but not bi-interpretable: equal strength is not the same as identity of theories. |