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Planck Length and Metric Geometry

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22 May 2025

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23 May 2025

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Abstract
The problem of Planck length is considered in the framework of metric geometry. A geodesic in the Gromov-Hausdorff space of isometry classes of compact metric spaces connecting a non-Archimedean with an Archimedean one is constructed.
Keywords: 
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1. The Planck Length Problem

The Planck length is the following combination of fundamental constants, having the dimension of length:
P l = G c 3 .
Numerical value of the Planck length is P l 1.61 · 10 33 c m .
The physical meaning of the Planck length is as follows. This is a scale on which it is fundamentally impossible to consider the theory of gravity without taking into account the quantum effects [1], since it is on the Planck scale that the values with the dimension of length inherent for gravity theory (the Schwarzschild radius of a spherically symmetric black hole) coincide with those for quantum theory (the Compton wavelength). Really, the Compton wavelength is given by the expression
λ C = m c ,
and the Schwarzschild radius is
r g = 2 G m c 2 .
It is easy to see that the equality takes place:
P l 2 = λ C r g 2 .
The appearance of a black hole on Planck scales does not allow us to obtain information about the structure of space on scales smaller than the Planck length.
In [2], it was conjectured that this kind of effect is associated with a fundamental change in the geometry of space on the Planck scale. Namely, the existence of unmeasurable regions of space is the result of a violation of Archimedes’ axiom (the axiom of measurability) in Euclidean geometry. A conjecture about the non-Archimedean nature of space on Planck scales was formulated. This gave rise to the development of a new field in mathematical physics [3,4].
However, the question of the mechanism of changing the metric from Archimedean to non-Archimedean remains open. In this paper, an attempt is made to construct a model of metric change using the apparatus of metric geometry. Namely, a geodesic in the Gromov-Hausdorff space connecting ultrametric and ordinary metric spaces will be explicitly constructed. As a model example of an ultrametric space, we will consider the set Z p of p-adic integers with a metric generated by the standard p-adic norm; as a model example of an ordinary metric space, we will choose the unit segment [ 0 , 1 ] R with a standard metric generated by the absolute value.

2. Metric Geometry. Basic Notions

A metric space is a pair X = ( X , d X ) , where X is a set, d X is a metric on X, that is, a mapping d X : X × X [ 0 , ) satisfying the conditions:
  • d X ( x , x ) = 0 x = x ;
  • d X ( x , x ) = d X ( x , x ) ;
  • d X ( x , x ) d X ( x , x ) + d X ( x , x ) .
If d X satisfies the condition d X ( x , x " ) max { d X ( x , x ) , d X ( x , x " ) } then this is ultrametric, the space ( X , d X ) is ultrametric (or non-Archimedean).
Important examples for the future are the following.
  • I = [ 0 , 1 ] , d I ( x , x ) = | x x | – Archimedean space;
  • Z p , d Z p ( x , x ) = | x x | p – non-Archimedean space;
  • Δ m = { x 1 , x m } , d Δ m ( x i , x j ) = 1 , i j , i , j = 1 , 2 , , m – simplex.
We define two operations on metric spaces: direct product and dilation.
Direct product ( X × Y , d X × Y ) of the metric spaces X and Y is the Cartesian product of X × Y with the metric given by the expression
d X × Y ( x , y ) , ( x , y ) = max d X ( x , x ) , d Y ( y , y ) .
Let λ R + be a positive real number. The space λ X obtained from the space ( X , d X ) by dilation the metric has the form:
λ X = ( X , λ d X ) .
Let ( X , d ) be a metric space and H = H ( X ) be a set of compact subsets of X. We define the metric (Hausdorff metric) d H on H.
Let A , B H ( X ) ,
d H ( A , B ) = inf { ϵ > 0 : B U ϵ ( A ) and A U ϵ ( B ) } ,
where U ϵ ( A ) = { x X : d ( x , A ) ϵ } .
( H ( X ) , d H ) is a metric space, and it is true that H ( X ) is compact if and only if X is compact.
By means of G H , we denote the set of isometric classes of compact metric spaces. We introduce the metric on the set G H as follows [5,6].
The realization of the pair X , Y of compact metric spaces is called the triple ( Z , X , Y ) , where Z is a metric space, X Z , Y Z , X , Y are isometric to X , Y , respectively, and d Z | X = d X , d Z | Y = d Y .
d G H ( X , Y ) = inf r e a l i z a t i o n s o f X , Y d H ( X , Y ) .
( G H , d G H ) is a complete separable metric space.

3. Calculation of Distances

The following Theorems are valid.
Theorem 1.
d G H ( I , Z p ) = 1 2 .
Theorem 2.
Let X be a connected compact metric space, diam X = 1 . Then we have:
d G H ( X , Z p ) = 1 2 .
Theorem 3.
Let k be a positive integer such that the inequalities p k < q < p k + 1 are satisfied. Then equality is valid:
2 d G H ( Z p , Z q ) = 1 1 p k .
A subset of R ( X , Y ) X × Y of the direct product of the sets X and Y is called a correspondence if the projections of this subset onto the components of the product are surjective: pr X R ( X , Y ) = X , pr Y R ( X , Y ) = Y .
The distortion dist R ( X , Y ) of a corresponence R ( X , Y ) is the following number:
dist R ( X , Y ) = sup ( x , y ) , ( x , y ) R ( X , Y ) | d X ( x , x ) d Y ( y , y ) |
.
The following statement [6] is true:
d G H ( X , Y ) = 1 2 inf c o r r e s p o n d e n c e s R ( X , Y ) dist R ( X , Y ) .
This statement provides a convenient way to calculate distances in the Gromov-Hausdorff space. Here are some simple examples.
Example 1.
Let R ( X , Y ) = X × Y , then
dist R ( X , Y ) = max { diam X , diam Y } .
Therefore,
2 d G H ( X , Y ) max { diam X , diam Y } .
Example 2.
2 d G H ( X , Δ 1 ) = diam X . Using the triangle inequality
d G H ( X , Δ 1 ) d G H ( X , Y ) + d G H ( Y , Δ 1 ) ,
we get:
2 d G H ( X , Y ) | diam X diam Y | .
Example 3.
Let f : X Y be surjective. Then the graph { ( x , f ( x ) ) , x X } is a correspondence.
There are two important points:
  • there is (not unique) optimal correspondence
    R o p t ( X , Y ) : 2 d G H = dist R o p t ( X , Y ) ;
  • to calculate distances in the Gromov-Hausdorff space, it is enough to consider only closed correspondences.
Proof of Theorem 1. Let R ( Z p , I ) be an arbitrary closed correspondence. Let’s consider Z p as a disjoint union of p balls of radius 1 / p , Z p = i = 1 , , p B 1 / p i . The family of subsets I of the form { pr I R ( B 1 / p i , I ) , i = 1 , , p } forms a covering of the segment I by closed subsets. Since I is connected, at least two sets of our coverage have a common point. The projections on Z p of the preimages of this common point lie in different balls B i and B j . Therefore, the distance in Z p between the projections of the preimages is equal to one. Thus, dist R ( Z p , I ) 1 . Since this is true for any correspondence, choosing the optimal one yields 2 d G H ( Z p , I ) 1 . On the other hand, 2 d G H ( Z p , I ) max { diam Z p , diam I } = 1 .
Since we used only the connectivity of the space I , the same proof works in the case of Theorem 2.
Proof of Theorem 3.
Let N be a positive integer. Let’s consider Z p as a disjoint union of p N balls of radius ϵ = p N . We will choose one point in each ball of the constructed partition. The set X N ( p ) obtained in this way, consisting of p N points, is provided with the metric d N , induced by the metric on Z p . As a result, we get the metric space ( X N ( p ) , d N ) . It is useful to note that the space X 1 ( p ) is nothing but a simplex of Δ p . Note that the Hausdorff distance between Z p and X N ( p ) is equal to ϵ . This immediately implies the validity of the evaluation of d G H ( Z p , X N ( p ) ) ϵ (it suffices to consider the realization of the pair ( Z p , X N ( p ) ) of the form Z = Z p = Y , X = X N ( p ) ).
The following simple Lemma follows from the triangle inequality.
Lemma 1.
For any metric compact X, the inequality holds:
d G H ( X , Z p ) d G H ( X , X N ( p ) ) p N .
Let M S T ( X N ( p ) ) be the minimum spanning tree of a finite metric space X N ( p ) . By means of σ ( X N ( p ) ) , we denote the mst-spectrum of the space X N ( p ) , that is, the sequence of edge lengths of the minimum spanning tree in decreasing order. The following Lemma is valid.
Lemma 2.
σ ( X N ( p ) ) = 1 , , 1 p 1 1 p , , 1 p p ( p 1 ) , 1 p 2 , , 1 p 2 p 2 ( p 1 ) , 1 p N 1 , , 1 p N 1 p N 1 ( p 1 ) .
Let’s decompose Z p into a disjoint union of p balls of radius 1 / p : Z p = i p B 1 / p i . In each of the partition balls, we will choose one element from the set X N ( p ) . The pairwise distances between the various elements of this set are equal to one, that is, it is a simplex Δ p . It follows directly from this that M S T ( X N ( p ) ) has exactly p 1 edge of length 1. Now each of the balls B 1 / p i , i = 1 , 2 , , p of our partition let’s decompose into disjoint union of p balls of radius 1 / p 2 (in total, we get p 2 balls of radius 1 / p 2 ) and let’s do a similar reasoning for each of these balls. Continuing these arguments N times, we obtain the statement of the Lemma.
To further prove of Theorem 3, we first prove the estimate from below:
1 1 p k 2 d G H ( Z p , Z q ) .
From the triangle inequality for the spaces Z p , Z q , Δ p k we obtain:
d G H ( Z p Z q ) d G H ( Δ p k , Z q ) d G H ( Δ p k , Z p ) .
Next, we will use the results of [7] (Theorem 3.3). The above theorem states, in particular, the following:
2 d G H ( Δ m , X ) = max { σ 1 1 , σ m , 1 σ m 1 } ,
where X is a finite ultrametric space consisting of n points, and 1 < m < n .
Let’s choose a positive integer N, q < p N . Then the equality
2 d G H ( Δ p k , X N ( q ) ) = 1
is valid, because σ 1 = σ p 1 = σ p k = 1 . In addition, the following equality is true
2 d G H ( Δ p k , X N ( p ) ) = 1 / p k ,
because in this case σ 1 = σ p 1 = 1 and σ p k = 1 / p k . Taking into account the last equalities for sufficiently large N, we obtain the required estimate from below.
To obtain an estimate from above, we construct the correspondence R ( Z p , Z q ) explicitly and calculate its distortion.
Let’s represent the number q as the sum of positive integers of the following form:
q = q 1 + q 2 + + q p k , 1 q i p , i = 1 , 2 , , p k .
Note that in this representation, at least one of the terms is not equal to 1 (since p k < q ).
Let’s decompose Z p into a disjoint union of p k balls of radius p k :
Z p = i = 1 p k B p k i .
Let’s represent Z q as a disjoint union of balls of radius q 1 in accordance with the above decomposition of the number q:
Z q = i 1 = 1 q 1 B q 1 i 1 i 2 = 1 q 2 B q 1 i 2 i 1 = 1 q p k B q 1 i p k .
Since any compact totally disconnected spaces are homeomorphic, there exists a homeomorphism ϕ : Z q Z p such that for all j = 1 , 2 , p k the conditions
ϕ i j = 1 q j B q 1 i j = B p k j
are fulfilled.
As the desired correspondence, R ( Z q , Z p ) let’s take the graph of the map ϕ .
We’ll show that the distortion of this correspondence is 1 1 p k .
Let x , x Z q : | x x | q 1 q , then the inequality | ϕ ( x ) ϕ ( x ) | p 1 p k is fulfilled by the definition of the map ϕ . Indeed, the inequality | x x | q 1 q means that x and x lie inside a ball of radius 1 / q , and the image of each such ball lies inside a ball of radius 1 / p k in Z p . Therefore, for all such x and x , the inequality | x x | q | ϕ ( x ) ϕ ( x ) | p p k holds.
Now let x and x lie in different balls of radius 1 / q in Z q (in this case, | x x | q = 1 ). There are two possible cases here. The first is when x and x lie in different groups of balls, and the second is when they lie in the same group of balls.
In the first case, we have | ϕ ( x ) ϕ ( x ) | p p k + 1 , since ϕ ( x ) and ϕ ( x ) lie in different balls of radius p k in Z p . Therefore, the inequality
| x x | q | ϕ ( x ) ϕ ( x ) | | p 1 p k + 1
holds.
In the second case, | ϕ ( x ) ϕ ( x ) | p p k , since ϕ ( x ) and ϕ ( x ) lie in the same ball of radius p k in Z p .
Now we will impose an additional condition on the map ϕ . As noted earlier, in our partition of a set consisting of q balls of radius 1 / q in Z q into p k groups of balls, there are groups (at least one) consisting of q k balls such that the inequalities 2 q k p are satisfied. The image of each such group under the map ϕ , is a ball of radius p k in Z p (each group has its own). Let’s decompose this ball into a disjoint union of p balls of radius p k 1 , and divide this set into q k groups (recall that q k p ). We will construct the map ϕ in such a way that each of the q k balls is mapped into its own group. In this case, if x and x lie in different balls from the group of q k balls, then their images lie in different balls of radius p k 1 inside a ball of radius p k and, thus, | ϕ ( x ) ϕ ( x ) | p = p k .
Thus, we have obtained the following properties of the map ϕ :
| x x | q | ϕ ( x ) ϕ ( x ) | p 1 p k , if | x x | q 1 q ,
and in the case of | x x | q = 1 :
| x x | q | ϕ ( x ) ϕ ( x ) | p 1 1 p k 1
or
| x x | q | ϕ ( x ) ϕ ( x ) | p = 1 1 p k .
It follows directly from the last formulas that the graph of the constructed map ϕ has a distortion equal to 1 1 p k . Therefore, the inequality is valid 2 d G H Z p , Z q 1 1 p k . The theorem has been proved.

4. Geodesics

Note that the correspondence constructed during the proof of theorem 3 (the graph of the map ϕ : Z q Z p ) is optimal.
It is not difficult to construct an optimal correspondence R ( Z p , I ) between Z p and the unit interval I .
As such a correspondence, consider the graph of the Monna map.
Let Z p x = x 0 + x 1 p + x k p k + . The Monna map μ : Z p I is given by the expression
μ ( x ) = 1 p ( x 0 + x 1 p 1 + + x k p k ) .
Calculate the distortion of the Monna map’s graph. Let x , x Z p : | x x | p = p n . This means that x 0 = x 0 , x 1 = x 1 , , x n 1 = x n 1 , x n x n . Then the inequality is valid
| μ ( x ) μ ( x ) | p n .
Therefore, for all x , x : | x x | < 1 , the estimate
| x x | p | μ ( x ) μ ( x ) | 1 / p
is valid.
Now let | x x | p = 1 , that is, x 0 x 0 . Let x 0 > x 0 be for certainty, then ( x x ) 0 = x 0 x 0 and the inequalities are valid
x 0 x 0 p | μ ( x ) μ ( x ) | x 0 x 0 + 1 p .
It immediately follows that the distortion of the Monna map’s graph is 1 1 p . Taking into account theorem 1, it can be concluded that the Monna map’s graph defines the optimal correspondence between Z p and I .
Our task is to construct a geodesic connecting Z p and I in the Gromov-Hausdorff space. To do this, we will use the following result from the paper [8]:
Proposition 1.
Let ( X , d X ) , ( Y , d Y ) be compact metric spaces, then for any optimal correspondence R o p t ( X , Y ) there is a family of compact metric spaces R t such that R 0 = X , R 1 = Y and for t ( 0 , 1 ) R t = R o p t ( X , Y ) , d t , where
d t ( x , y ) , ( x , y ) = ( 1 t ) d X ( x , x ) + t d Y ( y , y )
defines the shortest curve in G H connecting the spaces X and Y.
Thus, the following statement is true.
Theorem 4.
The family of spaces ( Z p , d 0 = | · | p ) , ( Γ μ , d t ) , ( I , d 1 = | · | ) , where Γ μ Z p × I denotes the graph of the Monna map,
d t ( x , μ ( x ) ) , ( y , μ ( y ) ) = ( 1 t ) | x y | p + t | μ ( x ) μ ( y ) | , t ( 0 , 1 ) ,
defines the shortest curve connecting Z p and I in the Gromov-Hausdorff space.
A geodesic connecting Z p and Z q is constructed in a similar way. To do this, instead of the graph of the Monna map, we need to take the graph of the map ϕ from the proof of theorem 3.

References

  1. D. Oriti, ed. Approaches to quantum gravity. Toward a new understanding of space, time and matter. Cambridge University Press, 2009.
  2. I. V. Volovich, Number Theory as the Ultimate Physical Theory, preprint CERN-TH. 4781/87, CERN, Geneva, 1987, 11 pp., reproduced in "p-Adic Numbers Ultrametric Anal. Appl. 2 (1), 77–87 (2010).
  3. V. S. Vladimirov, I. V. Volovich, E. I. Zelenov, p-Adic analysis and mathematical physics, Series on Soviet and East European Mathematics, 1, World Scientific Publishing Co. Inc., River Edge, NJ, 1994.
  4. B. Dragovich, A. Yu. Khrennikov, S. V. Kozyrev, I. V. Volovich, E. I. Zelenov. p-Adic Mathematical Physics: The First 30 Years, P-Adic Numbers Ultrametric Anal. Appl., 9:2 (2017), 87–121, arXiv: 1705.04758.
  5. M. Gromov. Metric structures for Riemannian and non-Riemannian spaces. Birkhäuser Boston, MA, 2007.
  6. D. Burago, Yu. Burago, S. Ivanov. A course in metric geometry. AMS, 2001.
  7. A. O. Ivanov, A. A. Tuzhilin. The Gromov-Hausdorff Distances between Simplexes and Ultrametric Spaces. arXiv:1907.03828v1, 2019. [CrossRef]
  8. A. O. Ivanov, S. Iliadis, A. A. Tuzhilin. Realization of Gromov-Hausdorff Distance. arXiv:1603.08850v1, 2016. [CrossRef]
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