⚜ PRINCIPIA ORTHOGONA · Vol VI · Roots · WP-106 ← WP-105 · The Unit That Inflates
Same ground, elsewhere in the series Bk4 · RH · Arithmetic Contact Structure · WP-96 · The Second Instrument · WP-103 · Why Six, and Why Not Five · WP-105 · The Unit That Inflates
#Derivation
Vol VI · Roots · WP-106 · Received 2026-09-08 · Tests the prototype of the RH paper §2 · Answers §9 question 3 in the negative · Novelty claimed, and only in §7

The Arithmetic Is in the Lattice

The RH paper asks whether the adelic contact form defines a contact topology, and calls the construction new. Before that question can be asked, a smaller one has to be answered: does a contact form over ℚp know anything a contact form over ℝ does not? At a point, no — and the reason closes the question permanently. On a lattice, yes, and the corpus’s own prototype is non-standard at exactly one place.
Methodexact Fraction and Smith-normal-form arithmetic, no floats
reproduced by wp106-verify.py
InputsCrespo & Pelayo 2024–2025 for the even-dimensional theory
Shimura 1963 for the arithmetic of alternating forms
Claim typetwo negative results, one positive one, and one gap in a vocabulary
the positive result is classical machinery in an unwritten place
Status§2–§6 settled and reproducible · §9 open
bears on the RH paper §5.2, not on §6
p-adic contact geometry” returns nothing because nobody has written it, and an empty shelf is an invitation to two different mistakes. The first is to assume the shelf is empty because the objects do not exist. The second is to assume it is empty because nobody got round to it. Here it is the second — the objects exist and behave — but the useful finding is where the arithmetic turns out to live, which is not where one would put it.
COMPUTED produced by the companion script CHECKED verified against a primary source OPEN not established here
The state of the field

§ 1 The even-dimensional half exists; the odd-dimensional half does not

p-adic symplectic geometry is four years old and has an author. Luis Crespo and Álvaro Pelayo have built it in a short sequence: the p-adic Jaynes–Cummings model (2024), integrable systems and Weierstrass–Williamson theory (January 2025), Darboux’s theorem (August 2025), and group actions (December 2025) CHECKED [1]–[4].

Three things in that work matter here. Their Theorem A is a p-adic Moser’s path method, and it needs a hypothesis the real one does not: the vector field’s components must vanish on the relevant compact set together with their partial derivatives. The real trick does not transfer unchanged. Their Theorem B is the local Darboux normal form. And their Theorem E is the one worth staring at — every second-countable 2n-dimensional p-adic analytic symplectic manifold is symplectomorphic to a union of balls determined entirely by volume. That is a global rigidity with no real analogue at all.

What is absent, across all four papers and Pelayo’s publication list, is any mention of contact structures, Reeb fields, Legendrian submanifolds or odd dimensions CHECKED. The programme is stated as even-dimensional and is carried out that way.

Why this note exists

The RH paper’s §9 question 3 says the construction of αarith on the adele class space is “to our knowledge, new”, and asks whether the space admits a contact topology — tight versus overtwisted. That question cannot be assessed while it is unknown whether a contact form over ℚp carries any arithmetic at all. This note settles the prior question and, in doing so, weakens the later one. That is the honest order.

Two things that survive

§ 2 The contact condition does not notice the change of field

The prototype of the RH paper §2 is

α = dz − r² dθ = dz + y dx − x dy,    dα = −2 dx ∧ dy,    α ∧ dα = −2 dx ∧ dy ∧ dz

and the standard model is α = dz − y dx, with α ∧ dα = dx ∧ dy ∧ dz. Both coefficients are nonzero rationals, so both are nonzero in every ℚp COMPUTED. This is not a coincidence of these two forms: α ∧ (dα)n ≠ 0 is an open algebraic condition, and a form that satisfies it over ℚ satisfies it over every completion. No place is excluded, and there is no p at which the prototype fails to be contact.

§ 3 The Reeb field survives; the question one asks after it does not

The Reeb field is defined by α(R) = 1 and ιR dα = 0. That is a linear system, and linear systems do not care what field they are over. For the prototype it returns R = ∂/∂z COMPUTED — the same answer Book 7 Ch Fy computes in the smooth case.

The next step in the real theory does not come with it, and this is the more useful half of the section. Over ℝ the Reeb field integrates to a flow, and the subject is closed orbits: Weinstein’s conjecture, Taubes’ theorem in dimension three. ℚp has no ℝ acting on it, and a p-adic analytic vector field integrates only on a ball of bounded radius. So “closed Reeb orbit” has no p-adic meaning as stated OPEN.

A vocabulary gap, not a theorem

The sentence above says that a question is not yet askable, which is weaker than saying the answer is no. Ch Fy already showed the smooth prototype has no closed Reeb orbit at all, so the analogy was not going to import anything even if it typechecked. Both facts point the same way and neither is a proof about αarith.

One thing that is not there

§ 4 There is no arithmetic at a point, and the reason is structural

The natural hope is that a contact structure over ℚp splits into classes the way a quadratic form does. Over ℚp the square classes are finite and few — four for odd p, eight for p = 2 COMPUTED — and they separate ⟨1,1⟩ from ⟨1,u⟩ for u a non-square. That is why p-adic orthogonal geometry is arithmetically rich.

Alternating forms have no such invariant, and the failure is explicit rather than an absence of proof. For a contact form the structure on H = ker α is a symplectic form up to scale, so the question is whether the multiplier is an invariant. It is not: for every λ there is a similitude realising it, and one can write it down.

S = diag(λ, …, λ, 1, …, 1)  ⇒   ST J S = λ J

Checked for n = 1, 2, 3 against every square class at p = 2, 3, 5, 7 — 60 cases, all solved COMPUTED. Scaling one Lagrangian half and leaving the other alone is available over any field, which is exactly why the multiplier carries no information.

Consequence — and it is a closure, not a step

p-adic contact linear algebra is as rigid as real contact linear algebra. Any hope that a contact structure over ℚp is arithmetically interesting at a point ends here, permanently. This is a negative result and it is the most load-bearing paragraph in the note, because it is what stops the next section from being read as more than it is.

Where it does live

§ 5 The lattice model, and the classical invariant on it

Arithmetic appears one level up. Take L a free ℤp-lattice model of rank 2n+1 and α a contact form on it. On H = ker α the form dα|H is alternating, and an alternating form over ℤp has elementary divisors, in equal pairs d1 | d1 | d2 | d2 | … This is Shimura’s Arithmetic of alternating forms, 1963 CHECKED [5]. A ℤp-analytic coordinate change has unit Jacobian and cannot move them; rescaling α by a constant c ∈ ℚp× shifts every valuation by vp(c) simultaneously.

So the invariant of the pair (lattice model, contact structure) is the multiset of valuations of those elementary divisors, taken modulo the simultaneous shift. Its coarse shadow is a single number, and it is the one worth carrying:

δp(α) = vp ( α ∧ (dα)n )   mod (n+1)

Well defined for the same two reasons: the top form scales by a unit determinant under a ℤp coordinate change, and by cn+1 under rescaling. On a rank-5 example — α = dz + (y1dx1 − x1dy1) + 3(y2dx2 − x2dy2) — it takes the values δ2 = 2 and δ3 = 1 COMPUTED, so it is not a parity and the group ℤ/(n+1) is genuinely used.

§ 6 The prototype is non-standard at p = 2, and at no other place

formelem. divisor valuations, p = 2p oddδ2δp, p odd
dz − y dx (standard)(0, 0)(0, 0)00
dz − r² dθ (prototype)(1, 1)(0, 0)10

The two rows differ at p = 2 and agree at 3, 5, 7, 11 COMPUTED. So the RH paper’s prototype is ℤp-isomorphic to the standard contact model at every odd place and is not at p = 2.

The invariant is not what convinces; the witness is. Over ℝ one standardises the prototype with

z′ = z + xy,   x′ = 2x  ⇒   α = dz′ − x′ dy

which the script verifies coefficient by coefficient. That substitution has determinant 2. It lies in GL3(ℤp) for odd p and not in GL3(ℤ2) COMPUTED. Invariant and witness agree, which is the only reason to trust either.

Worth saying plainly: the 2 comes from r²dθ = x dy − y dx being written antisymmetrically, and there is no dm³ content in it. A form that had been written −x dy would have δ2 = 0. That is a fact about the chart, not about the geometry — and it is precisely why δp is an invariant of a model and never of a manifold.

The register

§ 7 What is claimed as new, stated as narrowly as it deserves

statementstatus
Alternating forms over ℤp are classified by elementary divisorsClassical. Shimura, JMSJ 1963
Symplectic similitudes of every multiplier exist over any fieldClassical. Immediate from the symplectic basis theorem
Square classes of ℚp×; quadratic forms are separated by themClassical. Serre, A Course in Arithmetic, ch. III–IV
p-adic Darboux, Moser and the global ball classificationClassical, 2025. Crespo & Pelayo [3]; even-dimensional only
That contact forms over ℚp have been given none of thisObserved. Searched; no counter-instance found
§4: no arithmetic invariant at a point, with the similitude as witnessNew as written here, and elementary. Anyone who asked would get the same answer in an afternoon
§5: δp and the elementary-divisor invariant applied to a contact modelNew as written here. The machinery is Shimura’s; the application appears unwritten
§6: the prototype is non-standard exactly at p = 2New, and about this corpus’s own chart. Not a fact about anyone else’s geometry
Contact Darboux over ℚpOPEN not attempted here
The honest size of this

Nothing above required a new technique. The whole of §4 and §5 is what a specialist would produce on request, and the claim is only that nobody has been asked. “Unwritten” is a statement about a literature search, not about difficulty, and it is the weakest kind of novelty there is. It is still a novelty claim, and this note makes it in the three rows above and nowhere else.

What it is not

§ 8 What this does not say about αarith

It bears on the RH paper’s §5.2, the local contact forms, and on nothing after it. Three separations, in decreasing order of obviousness.

Category. The adele class space ℂ = 𝕊×/ℚ× is not a p-adic analytic manifold. It is the non-Hausdorff quotient that motivated Connes’ noncommutative treatment in the first place. Crespo and Pelayo’s category does not contain αarith, so their theorems do not apply to it and nothing here is transported to it.

Direction. §9 question 3 hopes that if αarith defines a tight contact structure, that would be a rigidity consistent with RH. If the contact analogue of Crespo–Pelayo’s Theorem E holds — global standardness — then there is no tight/overtwisted dichotomy over ℚp and the hoped-for statement has no content at the finite places. That would be a negative answer to the paper’s own question, and the paper should carry it as such rather than leaving the question open in a form that cannot come back either way OPEN.

Scale. Nothing here bounds anything, computes anything about ζ, or bears on §6 global positivity. The last row of the RH paper’s status table is unchanged by this note, and so is every row above it.

The temptation this note is written against

“Contact structure” and “p-adic” can be put in one sentence without either word doing work, and the resulting sentence sounds like a programme. The test applied throughout was whether a computation could come back empty. §4 came back empty and is reported as such; §6 came back with one place and not a family. A construction that produced an interesting invariant at every prime would have been the warning sign, not the result.

§ 9 What would have to be done next

  1. Contact Darboux over ℚp. The tool exists — Crespo & Pelayo’s Theorem A, p-adic Moser with the strengthened vanishing hypothesis. The real proof of contact Darboux runs through Gray stability and should transfer under the same hypothesis. Until it is done, §5 classifies models and not germs. OPEN
  2. The global question. Whether the contact analogue of Theorem E holds — every second-countable p-adic contact manifold standard, hence no tight/overtwisted dichotomy. This is the statement that would settle §8, and it is the one worth the effort. OPEN
  3. The local forms of the RH paper §5.2. Whether αp admits a ℤp-lattice model at all, and if so what δp is. If it is nonzero at finitely many places, that set is a conductor and deserves the name. If it is nonzero at infinitely many, the model is the wrong one. Either outcome is informative, which is the reason to compute it. OPEN

§ 10 Sources

[1] L. Crespo & Á. Pelayo, The p-adic Jaynes–Cummings model in symplectic geometry, arXiv:2406.18415 (2024).
[2] L. Crespo & Á. Pelayo, p-adic symplectic geometry of integrable systems and Weierstrass–Williamson theory, arXiv:2501.14444 (2025).
[3] L. Crespo & Á. Pelayo, Darboux’s Theorem in p-adic symplectic geometry, arXiv:2508.15443 (2025). Theorems A, B, C and E as cited in §1.
[4] L. Crespo & Á. Pelayo, Group actions on p-adic symplectic manifolds, arXiv:2512.15575 (2025).
[5] G. Shimura, Arithmetic of alternating forms and quaternion hermitian forms, J. Math. Soc. Japan 15 (1963), 33–65.
[6] J.-P. Serre, A Course in Arithmetic, Springer GTM 7, ch. III–IV, for the square classes of ℚp× and the classification of quadratic forms.
[7] This corpus: RH_arithmetic_contact_structure.md §2, §5.2, §9 (rendered at book4/rh-paper.html); book7 Ch Fy for the smooth Reeb computation; book6/wp96-the-second-instrument.html for the two-column instrument argument this note reuses in §4.
[8] Every number in this note is regenerated by wp106-verify.py (sympy 1.14; exact Fraction and Smith normal form; all checks pass).