Construction of a set of p-adic distributions
U. A. Rozikov, Z. T. Tugyonov

TL;DR
This paper develops methods to construct $p$-adic distributions on $Z_p$, adapting real-valued Gibbs measure techniques, and identifies conditions for these distributions to be bounded measures.
Contribution
It introduces a novel approach to constructing $p$-adic distributions on $Z_p$ inspired by Gibbs measures on Cayley trees, extending existing methods.
Findings
Constructed several $p$-adic distributions on $Z_p$
Provided conditions for these distributions to be $p$-adic measures
Extended real-valued Gibbs measure techniques to the $p$-adic setting
Abstract
In this paper adapting to -adic case some methods of real valued Gibbs measures on Cayley trees we construct several -adic distributions on the set of -adic integers. Moreover, we give conditions under which these -adic distributions become -adic measures (i.e. bounded distributions).
Click any figure to enlarge with its caption.
Figure 1
Figure 2Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Construction of a set of p-adic distributions
U. A. Rozikov, Z. T. Tugyonov
U. A. Rozikov and Z. T. Tug’yonov
Institute of mathematics, 29, Do’rmon Yo’li str., 100125, Tashkent, Uzbekistan.
[email protected] [email protected]
Abstract.
In this paper adapting to -adic case some methods of real valued Gibbs measures on Cayley trees we construct several -adic distributions on the set of -adic integers. Moreover, we give conditions under which these -adic distributions become -adic measures (i.e. bounded distributions).
Mathematics Subject Classifications (2010). 46S10, 82B26, 12J12 (primary); 60K35 (secondary)
Key words. Cayley trees, -adic numbers, -adic distributions, -adic measures.
1. Introduction
A -adic distribution is an analogue of ordinary distributions that takes values in a ring of -adic numbers [13]. Analogically to a measure on a measurable space, a -adic measure is a special case of a -adic distribution, i.e., a p-adic distribution taking values in a normed space is called a -adic measure if the values on compact open subsets are bounded.
The main purpose for constructing -adic measures is to integrate -adic valued functions. The development parallels the classic treatment, beginning with the idea of Riemann sums. Note that such sums may not converge (even for continuous functions) if instead of -adic measures one uses unbounded -adic distributions. The theory of -adic measures also useful in the context of -adic -functions following the works of B. Mazur (see [13] and [6] for details).
One of the first applications of -adic numbers in quantum physics appeared in the framework of quantum logic [2]. Note that this model cannot be described by using conventional real-valued probability measures. In (real valued probability) measure theory Kolmogorov’s extension theorem (see, e.g., [23, Ch. II]) is very helpful to construct measures.
A non-Archimedean analogue of the Kolmogorov’s theorem was proved in [5]. Such a result allows to construct wide classes of -adic distributions, stochastic processes and the possibility to develop statistical mechanics in the context of -adic theory.
We refer the reader to [4], [8], [11],[10]-[19] where various -adic models of statistical physics and -adic distributions are studied.
In the present paper we construct several -adic distributions and measures on the set of -adic integers. We use some arguments of construction of real valued Gibbs measures on Cayley trees. To do this we present each element of the set by a path in the half (semi-infinite) Cayley tree. Then using known distribution relation (see equation (2.2) below) we show that each collection of given -adic distributions can be used to construct new distributions. Moreover, we give conditions under which these -adic distributions become -adic measures.
2. Preliminaries
2.1. -adic numbers.
Let be the field of rational numbers. For a fixed prime number , every rational number can be represented in the form , where , is a positive integer, and and are relatively prime with : , . The -adic norm of is given by
[TABLE]
This norm is non-Archimedean and satisfies the so called strong triangle inequality
[TABLE]
The completion of with respect to the -adic norm defines the -adic field . Any -adic number can be uniquely represented in the canonical form
[TABLE]
where and the integers satisfy: , . In this case .
The elements of the set are called -adic integers.
We refer the reader to [13, 22, 27] for the basics of -adic analysis and -adic mathematical physics.
2.2. -adic distribution and measure
Let be a measurable space, where is an algebra of subsets of . A function is said to be a -adic distribution if for any such that , , the following holds:
[TABLE]
A -adic distribution is called measure if it is bounded, i.e.
[TABLE]
A measure is called a probability measure if , see, e.g. [9], [20].
In the metric space (with metric ) basis of open sets can be taken as the following system of sets:
[TABLE]
Such a set is called an interval. The following theorem is known:
Theorem 1**.**
(see [13]) Every map of the set of intervals contained in , for which
[TABLE]
for any , can be uniquely extended to a -adic distribution on .
Equation (2.2) is called a distribution relation.
Remark 1**.**
If are given distributions with values in and are arbitrary constants. Then
[TABLE]
is a distribution. Indeed, define
[TABLE]
then satisfies (2.2) since each satisfies (2.2). In the theory of real valued measures if one considers a convex set of such measures then to describe all points of this set it will be sufficient to know all extreme points of the set. In such a situations measures of the form (2.3) are not extreme and can be considered as linear combination of extreme measures. In the theory of (real) Gibbs measures for a given Hamiltonian (see [7] for details) the set of all such measures is a convex compact set. To construct new extreme points of this set in [3] the authors used some known extreme points. In this paper we will use idea of [3] to construct (see Theorem 2 below) new -adic distributions from the known ones. Proof of Theorem 3 also reminds the construction of a limiting Gibbs measure with a given boundary condition on a Cayley tree (see [21] for details of the theory of Gibbs measures on trees).
2.3. Cayley tree.
The Cayley tree (Bethe lattice [1]) of order is an infinite tree, i.e., a graph without cycles, such that exactly edges originate from each vertex. Let where is the set of vertices and the set of edges. Two vertices and are called nearest neighbors if there exists an edge connecting them. We will use the notation . A collection of nearest neighbor pairs is called a path from to . The distance on the Cayley tree is the number of edges of the shortest path from to .
If an arbitrary edge is deleted from the Cayley tree , it splits into two components– two semi-infinite trees and (each of which is called a half tree). In this paper we consider half tree (see Fig. 1).
For a fixed , called the root, we set
[TABLE]
On the tree one can introduce a partial ordering, by saying that if there exists a path from to that “goes upwards”, i.e., such that The set of vertices and the edges connecting them form the semi-infinite tree “growing” from the vertex .
Let be a prime number. In this paper we consider the half Cayley tree of order . Take an arbitrary (finite or infinite) path on starting from the point . We can represent the path by a sequence , where . Namely, we label by the edges going upward from the vertex . Then the path can be assigned a sequence such that , ; the sequence unambiguously determines the path .
A finite path of length determines a point . If the path is represented by the sequence , we assume that the vertex is also represented by this sequence (see Fig. 1).
Let , and let be represented by the sequence and by , where , ,…, , but for some . In this case, we write . Similarly, for pathes represented by a sequence and represented by , we write if , ,…, , but for some .
Let be an infinite path, represented by the sequence . We assign the -adic number
[TABLE]
to the path . This assignment is a 1-1 correspondence. Moreover, the partial order on the set of paths can be used to obtain partial order on : namely, for we write iff they correspond to , with .
3. Construction of distributions
Several examples of -adic distributions are known: Haar’s, Mazur’s, Bernoulli’s distributions etc.[13]. Recently some periodic distributions were constructed in [24]-[26].
Here for any two -adic distribution given on , say and , we construct a new distribution defined on .
Fix a path with representation . Take . If there exists such that has representation with , then we denote this by . We say that two pathes starting from has non-empty intersection if they have at least one common edge.
Theorem 2**.**
Let be an infinite path, represented by the sequence and , are given distributions on such that ,
[TABLE]
then there is a distribution on , which on the intervals is defined as follows
[TABLE]
where and is the path representing (see Fig. 1).
Proof.
Consider the following (all possible) cases:
Case I: . In this case the path always remains on the “left side” (i.e. ) or always on the “right side” (i.e. ) from the path . For any and any the number (present in formula (2.2)) makes contributions only on levels , , … of the branch growing from the vertex of the edge numbered by , (where ) of the tree . We note that does not intersect with . Consequently we have . By definition of given in (3.2) in case and for any one easily checks that always coincides with (or ), hence it satisfies the distribution relation (2.2).
In case , the exists such that , i.e. , where is the first number in the presentation of . In this case assuming the equality (2.2) can be written as
[TABLE]
Since the equality (2.2) is true for , the equality (3.3) is satisfied iff
[TABLE]
The last equality is true by condition (3.1).
Let now then the equality (2.2) can be written as
[TABLE]
Similarly as the case we obtain condition (3.4).
Case II: . In this case there exists such that has representation with .
Subcase : Since the path does not intersect with , the equation (2.2) for is
[TABLE]
[TABLE]
and
[TABLE]
[TABLE]
Since both and are distributions the last two equalities are true.
Subcase : In this case by our condition (3.1) we have , consequently, the distribution relation (2.2) is satisfied. ∎
The following theorem says that one can construct a new distribution using a collection of given distributions.
Theorem 3**.**
Let be a natural number. Assume for each a distribution on is given and there exists an interval , such that for at least one pair , . Then there exists a distribution on which is different from for each .
Proof.
The distribution can be constructed as follows (see Fig. 2).
Case: . Recall is the set of vertices in the semi-infinite tree growing from the vertex . In the case if , for some then also remains in for any . Therefore we define
[TABLE]
then
[TABLE]
Since is a given distribution the equation (2.2) is satisfied.
Case: . Without loss of generality we define only for which has the form
[TABLE]
where . Note that the sequence presents a unique point of .
For define
[TABLE]
[TABLE]
Now using formula (3.7) we define (for )
[TABLE]
[TABLE]
Iterating this procedure we recurrently define
[TABLE]
[TABLE]
where .
From the equalities (3.6)-(3.9) it follows that satisfies (2.2) for any and any . Therefore, by Theorem 2 it follows that can be uniquely extended to a -adic distribution on .
Now we show that is different from for any . Let us assume the converse, i.e. there exists such that . This means that for any and any we have
[TABLE]
For any there exists such that . Consequently, from (3.6) and (3.10) we get
[TABLE]
When runs arbitrary takes all values on . Therefore from (3.11) we get that , for any . But this is contradiction to the condition of theorem for and . Thus it follows that for each . This completes the proof. ∎
Remark 2**.**
We note that the distribution mentioned in Theorem 3 is useful to construct two distributions and which satisfy the condition of Theorem 2. Indeed, let and , consider such that , for some and . Define , by
[TABLE]
Take and , it is easy to check that and they satisfy the condition of Theorem 2.
In the -adic integral theory one need to -adic measure. Because integral of a continuous function calculated with respect to unbounded -adic distribution may not exist (see [13] for details).
In the following theorem we give a conditions under which -adic distributions mentioned in Theorems 2 and 3 become -adic measures.
Theorem 4**.**
The following statements hold
Distribution , mentioned in Theorem 2, is bounded iff and are bounded.
- 2)
Distribution , mentioned in Theorem 3, is bounded iff is bounded for each and .
Proof.
-
This is consequence of the equality (3.2).
-
Case : In this case from (3.6) we get that is bounded iff is bounded for each .
Case : Since the right hand side of (3.7) is sum of bounded terms (corresponding to the case ) the left hand side also should be bounded. Consequently, iterating of the recursions (3.7)-(3.9) one can see that is bounded iff is bounded for each and . ∎
Acknowledgements
This work was partially supported by Kazakhstan Ministry of Education and Science, grant 0828/GF4.
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] Baxter R.J. Exactly Solved Models in Statistical Mechanics (Academic, London, 1982).
- 2[2] Beltrametti E.G., Cassinelli G., Quantum Mechanics and p 𝑝 p -adic Numbers, Found. Phys. 2 , (1972), 1-7.
- 3[3] Bleher P.M., Ganikhodjaev N.N. On pure phases of the Ising model on the Bethe lattice. Theor. Probab. Appl. 35 (1990), 216-227.
- 4[4] Gandolfo G., Rozikov U.A., Ruiz J. On p 𝑝 p -adic Gibbs measures for hard core model on a Cayley tree. Markov Processes Related Fields . 18 (4) (2012), 701-720.
- 5[5] Ganikhodjaev N.N., Mukhamedov F.M., Rozikov U.A., Phase Transitions in the Ising Model on Z 𝑍 Z over the p 𝑝 p -adic Number Field, Uzb. Mat. Zh. , No. 4, (1998), 23-29.
- 6[6] Gras Georges, Mesures p 𝑝 p -adiques. (French) Théorie des nombres, Année 1991/1992, 107 pp., Publ. Math.Fac. Sci. Besançon, Univ. Franche-Comté, Besançon.
- 7[7] Georgii H.-O., Gibbs Measures and Phase Transitions (W. de Gruyter, Berlin, 1988).
- 8[8] Khamraev M., Mukhamedov F.M., Rozikov U.A. On the uniqueness of Gibbs measures for p − limit-from 𝑝 p- adic non homogeneous λ − limit-from 𝜆 \lambda- model on the Cayley tree. Letters in Math. Phys. 70 (2004), 17-28.
