Recognition: 2 theorem links
· Lean TheoremThe Haar measure of the p-adic rotation group textrm{SO}(3)_p via nautical angles
Pith reviewed 2026-05-08 19:29 UTC · model grok-4.3
The pith
The normalized Haar measure on the p-adic rotation group SO(3)_p is expressed explicitly as a factorized density in its three nautical angles.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Exploiting its topological group isomorphism with the quotient of p-adic quaternions by scalars, the corresponding change of variables formulas and the associated Jacobian are derived in the p-adic setting. This is combined with the known Haar measure on the multiplicative group of p-adic quaternions to yield an explicit formula for the normalized Haar measure on SO(3)_p in nautical coordinates with a factorized density in the three angles.
What carries the argument
The topological group isomorphism SO(3)_p ≅ H_p^x / Q_p^x together with the p-adic change-of-variables Jacobian for the nautical parametrization, which transports the Haar measure from the quaternion group.
If this is right
- The Haar integral over SO(3)_p reduces to an ordinary triple integral over the angle ranges with the explicit product density.
- Any continuous function on the group can be integrated using this coordinate expression of the measure.
- The normalization ensures the total measure is 1.
- This holds for every prime p, giving a uniform expression across all p-adic cases.
Where Pith is reading between the lines
- Analogous constructions might work for other p-adic compact groups admitting quaternion-like descriptions.
- The factored form could simplify the computation of characters or representation theory integrals on this group.
- Implementations in computer algebra systems could use this to sample from the invariant measure on p-adic rotations.
- Connections to p-adic special functions or orthogonal polynomials might be explored using this measure.
Load-bearing premise
The isomorphism between SO(3)_p and the quotient of the multiplicative p-adic quaternions by the scalars correctly transports the Haar measure when combined with the computed Jacobian.
What would settle it
Directly integrating the constant function 1 over the proposed measure and checking whether the result equals 1, or computing the measure of a known subset in two different ways.
read the original abstract
We study the explicit construction of the Haar measure on the compact $p$-adic rotation group $\textrm{SO}(3)_p$ by nautical (Cardano) parametrization. Exploiting its topological group isomorphism with $\mathbb{H}_p^\times/\mathbb{Q}_p^\times$ of $p$-adic quaternions modulo scalars, we derive the corresponding change of variables formulas and compute the associated Jacobian in the $p$-adic setting, which we combine with the known Haar measure on the multiplicative group of $p$-adic quaternions $\mathbb{H}_p^\times$. This yields an explicit formula for the normalized Haar measure on $\textrm{SO}(3)_p$ in nautical coordinates, with a factorized density in the three angles. Our construction provides a concrete tool suited for applications of non-Archimedean models where an explicit angular description of invariant integration is required.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript derives an explicit formula for the normalized Haar measure on the compact p-adic rotation group SO(3)_p in nautical (Cardano) angles. It exploits the topological group isomorphism SO(3)_p ≅ H_p^x / Q_p^x, obtains the corresponding p-adic change-of-variables formulas and Jacobian, and transports the known Haar measure on the multiplicative group H_p^x to produce a factorized density in the three angles.
Significance. If the explicit Jacobian and normalization are correctly computed, the result supplies a concrete angular parametrization of invariant integration on SO(3)_p. This is a useful tool for non-Archimedean models that require explicit angular descriptions, extending classical rotation-group techniques to the p-adic setting.
major comments (1)
- The central claim requires that the derived density integrate to one with respect to the p-adic measure on the parameter domain. The manuscript should supply this explicit normalization integral (or a reference to its evaluation) to confirm the measure is properly normalized rather than merely proportional.
minor comments (3)
- The abstract states that the Jacobian is computed but does not display the final expression; including the explicit p-adic Jacobian determinant in the abstract or a dedicated equation would improve immediate readability.
- Notation for the p-adic absolute value |·|_p and the domain of the nautical angles should be introduced with a brief reminder of their ranges in the p-adic topology.
- A short reference to the standard proof of the topological isomorphism SO(3)_p ≅ H_p^x / Q_p^x would help readers who are not already familiar with the quaternion construction.
Simulated Author's Rebuttal
We thank the referee for the careful reading and the recommendation of minor revision. The manuscript constructs the normalized Haar measure on SO(3)_p by transporting the known normalized Haar measure on H_p^x via the group isomorphism and the p-adic change-of-variables formula. We address the single major comment below.
read point-by-point responses
-
Referee: The central claim requires that the derived density integrate to one with respect to the p-adic measure on the parameter domain. The manuscript should supply this explicit normalization integral (or a reference to its evaluation) to confirm the measure is properly normalized rather than merely proportional.
Authors: We agree that an explicit verification strengthens the presentation. The normalization is inherited from the normalized Haar measure on H_p^x together with the Jacobian factor arising from the change of variables, but the manuscript does not display the resulting integral over the nautical-angle domain. In the revised version we will add a short subsection that evaluates this integral directly, using the factorized form of the density and the product structure of the p-adic parameter domain, thereby confirming that the total mass equals one. revision: yes
Circularity Check
Derivation self-contained from known Haar measure and isomorphism
full rationale
The paper begins with the established topological group isomorphism SO(3)_p ≅ H_p^x / Q_p^x and the known Haar measure on the multiplicative group H_p^x. It then derives the p-adic change-of-variables formulas and Jacobian to transport the measure to nautical coordinates, yielding an explicit factorized density. No load-bearing step reduces the final formula to a fitted input, self-definition, or self-citation chain; the central result follows from standard p-adic group theory and analysis without internal circularity.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption SO(3)_p is topologically isomorphic to H_p^x / Q_p^x as compact groups
- standard math A normalized Haar measure on H_p^x is known and bi-invariant
Lean theorems connected to this paper
-
IndisputableMonolith.Foundation.AlexanderDuality (D=3 forcing in the Archimedean spacetime chain)alexander_duality_circle_linking unclearWe study the explicit construction of the Haar measure on the compact p-adic rotation group SO(3)_p by nautical (Cardano) parametrization. Exploiting its topological group isomorphism with H_p^× / Q_p^× ...
-
IndisputableMonolith.Cost (J-cost ½(x+x⁻¹)−1)Jcost / washburn_uniqueness_aczel uncleardμ_SO(3)_p(R(α,β,γ)) = |dα dβ dγ / ((1−vα²)(1+pβ²)(1−(p/v)γ²))|_p
Reference graph
Works this paper leans on
-
[1]
Serre,A Course in Arithmetic, Graduate Studies in Mathematics7, Springer, 1973
J-P. Serre,A Course in Arithmetic, Graduate Studies in Mathematics7, Springer, 1973
1973
-
[2]
The wave function of the universe and p-adic gravity
L. Y. Araf’eva, B. Dragovich, P. H. Frampton, and I. V. Volovich, “The wave function of the universe and p-adic gravity”, Int. J. Mod. Phys. A6(24), pp. 4341–4358 (1991),https: //doi.org/10.1142/S0217751X91002094
-
[3]
P. G. O. Freund and E. Witten, “Adelic string amplitudes”, Phys. Lett. B199(2), pp. 191–194 (1987),https://doi.org/10.1016/0370-2693(87)91357-8
-
[4]
p-adic space-time and string theory
I. V. Volovich, “p-adic space-time and string theory”, Theor. Math. Phys.71(3), pp. 574–576 (1987),https://doi.org/10.1007/BF01017088
-
[5]
An approach top-adic qubits from irreducible representations of SO(3)p
I. Svampa, S. Mancini, and A. Winter, “An approach top-adic qubits from irreducible representations of SO(3)p”,J. Math. Phys.63(7), 072202 (2022),https://doi.org/10.1063/ 5.0089077. 16
2022
-
[6]
Ap-adic model of quantum states and thep-adic qubit
P. Aniello, S. Mancini, and V. Parisi, “Ap-adic model of quantum states and thep-adic qubit”, Entropy25(1), 86 (2023),https://doi.org/10.3390/e25010086
-
[7]
I. Svampa, S. L’Innocente, S. Mancini, and A. Winter, “Composingp-adic qubits: from representations of SO(3) p to entanglement and universal quantum logic gates”,https:// arxiv.org/abs/2601.13808
-
[8]
Quantum mechanics on ap-adic Hilbert space: foun- dations and prospects
P. Aniello, S. Mancini, and V. Parisi, “Quantum mechanics on ap-adic Hilbert space: foun- dations and prospects”,IJGMMP21, 2440017 (2024)
2024
-
[9]
Towards a p-adic model of quantum information theory
V. Parisi, “Towards a p-adic model of quantum information theory”, PhD thesis, Universit` a degli Studi di Napoli Federico II, March 2024,http://www.fedoa.unina.it/id/eprint/ 15492
2024
-
[10]
Geometry of the p-adic special orthogonal group SO(3) p
S. Di Martino, S. Mancini, M. Pigliapochi, I. Svampa, and A. Winter, “Geometry of the p-adic special orthogonal group SO(3) p”,Lobachevskii J. Math.44(6), pp. 2135–2159 (2023), https://doi.org/10.1134/S1995080223060355
-
[11]
G. B. Folland,A Course in Abstract Harmonic Analysis, CRC Press, 2016
2016
-
[12]
G. B. Folland,Real Analysis, Pure and Applied Mathematics, Wiley Series of Texts, Mono- graphs, and Tracts, John Wiley & Sons, 1999
1999
-
[13]
Invariant measures onp-adic Lie groups: thep-adic quaternion algebra and the Haar integral on thep-adic rotation groups
P. Aniello, S. L’Innocente, S. Mancini, V. Parisi, I. Svampa, and A. Winter, “Invariant measures onp-adic Lie groups: thep-adic quaternion algebra and the Haar integral on thep-adic rotation groups”,Lett. Math. Phys.114, 78 (2024),https://doi.org/10.1007/ s11005-024-01826-8
2024
-
[14]
Characterising the Haar measure on thep-adic rotation groups via inverse limits of measure spaces
P. Aniello, S. L’Innocente, S. Mancini, V. Parisi, I. Svampa, and A. Winter, “Characterising the Haar measure on thep-adic rotation groups via inverse limits of measure spaces”, Expo. Math.43(2), 125592 (2025),https://doi.org/10.1016/j.exmath.2024.125592
-
[15]
T. Y. Lam,Introduction to Quadratic Forms over Fields, Graduate Studies in Mathematics 67, American Mathematical Society, 2005
2005
-
[16]
Representations of thep-adic three-dimensional rotation group: to- wardsp-adic quantum computing
I. Svampa, “Representations of thep-adic three-dimensional rotation group: to- wardsp-adic quantum computing”, PhD thesis, Universit` a di Camerino and Universi- tat Aut` onoma de Barcelona, March 2025,https://pubblicazioni.unicam.it/retrieve/ d8920d9a-3a4c-4a9a-b910-1dbbce699359/Svampa_Tesi_PhD.pdforhttps://ddd.uab. cat/pub/tesis/2025/hdl_10803_694069/is1de1.pdf
2025
-
[17]
A. N. Kochubei,Pseudo-differential equations and stochastics over non-Archimedean fields, Monographs and Textbooks in pure and applied mathematics244, Marcel Dekker, 2001
2001
-
[18]
Voight,Quaternion Algebras, Graduate Texts in Mathematics288, Springer, 2011
J. Voight,Quaternion Algebras, Graduate Texts in Mathematics288, Springer, 2011
2011
-
[19]
Helgason,Differential Geometry, Lie Groups, and Symmetric Spaces, 1978
S. Helgason,Differential Geometry, Lie Groups, and Symmetric Spaces, 1978. 17
1978
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.