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Infinite divisibility
Infinite divisibility
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Infinite divisibility arises in different ways in philosophy, physics, economics, order theory (a branch of mathematics), and probability theory (also a branch of mathematics). One may speak of infinite divisibility, or the lack thereof, of matter, space, time, money, or abstract mathematical objects such as the continuum.

In philosophy

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The origin of the idea in the Western tradition can be traced to the 5th century BCE starting with the Ancient Greek pre-Socratic philosopher Democritus and his teacher Leucippus, who theorized matter's divisibility beyond what can be perceived by the senses until ultimately ending at an indivisible atom. The Indian philosopher, Maharshi Kanada also proposed an atomistic theory, however there is ambiguity around when this philosopher lived, ranging from sometime between the 6th century to 2nd century BCE. Around 500 BC, he postulated that if we go on dividing matter (padarth), we shall get smaller and smaller particles. Ultimately, a time will come when we shall come across the smallest particles beyond which further division will not be possible. He named these particles Parmanu. Another Indian philosopher, Pakudha Katyayama, elaborated this doctrine and said that these particles normally exist in a combined form which gives us various forms of matter.[1] [2] Atomism is explored in Plato's dialogue Timaeus. Aristotle proves that both length and time are infinitely divisible, refuting atomism.[3] Andrew Pyle gives a lucid account of infinite divisibility in the first few pages of his Atomism and its Critics. There he shows how infinite divisibility involves the idea that there is some extended item, such as an apple, which can be divided infinitely many times, where one never divides down to point, or to atoms of any sort. Many philosophers[who?] claim that infinite divisibility involves either a collection of an infinite number of items (since there are infinite divisions, there must be an infinite collection of objects), or (more rarely), point-sized items, or both. Pyle states that the mathematics of infinitely divisible extensions involve neither of these — that there are infinite divisions, but only finite collections of objects and they never are divided down to point extension-less items.

In Zeno's arrow paradox, Zeno questioned how an arrow can move if at one moment it is here and motionless and at a later moment be somewhere else and motionless.

Zeno's reasoning, however, is fallacious, when he says that if everything when it occupies an equal space is at rest, and if that which is in locomotion is always occupying such a space at any moment, the flying arrow is therefore motionless. This is false, for time is not composed of indivisible moments any more than any other magnitude is composed of indivisibles.[4]

— Aristotle, Physics VI:9, 239b5

In reference to Zeno's paradox of the arrow in flight, Alfred North Whitehead writes that "an infinite number of acts of becoming may take place in a finite time if each subsequent act is smaller in a convergent series":[5]

The argument, so far as it is valid, elicits a contradiction from the two premises: (i) that in a becoming something (res vera) becomes, and (ii) that every act of becoming is divisible into earlier and later sections which are themselves acts of becoming. Consider, for example, an act of becoming during one second. The act is divisible into two acts, one during the earlier half of the second, the other during the later half of the second. Thus that which becomes during the whole second presupposes that which becomes during the first half-second. Analogously, that which becomes during the first half-second presupposes that which becomes during the first quarter-second, and so on indefinitely. Thus if we consider the process of becoming up to the beginning of the second in question, and ask what then becomes, no answer can be given. For, whatever creature we indicate presupposes an earlier creature which became after the beginning of the second and antecedently to the indicated creature. Therefore there is nothing which becomes, so as to effect a transition into the second in question.[5]

— A.N. Whitehead, Process and Reality

In quantum physics

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Until the discovery of quantum mechanics, no distinction was made between the question of whether matter is infinitely divisible and the question of whether matter can be cut into smaller parts ad infinitum.

As a result, the Greek word átomos (ἄτομος), which literally means "uncuttable", is usually translated as "indivisible". Whereas the modern atom is indeed divisible, it actually is uncuttable: there is no partition of space such that its parts correspond to material parts of the atom. In other words, the quantum-mechanical description of matter no longer conforms to the cookie cutter paradigm.[6] This casts fresh light on the ancient conundrum of the divisibility of matter. The multiplicity of a material object—the number of its parts—depends on the existence, not of delimiting surfaces, but of internal spatial relations (relative positions between parts), and these lack determinate values. According to the Standard Model of particle physics, the particles that make up an atom—quarks and electrons—are point particles: they do not take up space. What makes an atom nevertheless take up space is not any spatially extended "stuff" that "occupies space", and that might be cut into smaller and smaller pieces, but the indeterminacy of its internal spatial relations.

Physical space is often regarded as infinitely divisible: it is thought that any region in space, no matter how small, could be further split. Time is similarly considered as infinitely divisible.

However, according to the best currently accepted theory in physics, the Standard Model, there is a distance (called the Planck length, 1.616229(38)×10−35 metres, named after one of the fathers of Quantum Theory, Max Planck) and therefore a time interval (the amount of time which light takes to traverse that distance in a vacuum, 5.39116(13) × 10−44 seconds, known as the Planck time) at which the Standard Model is expected to break down – effectively making this the smallest physical scale about which meaningful statements can be currently made. To predict the physical behaviour of space-time and fundamental particles at smaller distances requires a new theory of Quantum Gravity, which unifies the hitherto incompatible theories of Quantum Mechanics and General Relativity. [citation needed]

In economics

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One dollar, or one euro, is divided into 100 cents; one can only pay in increments of a cent. It is quite commonplace for prices of some commodities such as gasoline to be in increments of a tenth of a cent per gallon or per litre. If gasoline costs $3.979 per gallon and one buys 10 gallons, then the "extra" 9/10 of a cent comes to ten times that: an "extra" 9 cents, so the cent in that case gets paid. Money is infinitely divisible in the sense that it is based upon the real number system. However, modern day coins are not divisible (in the past some coins were weighed with each transaction, and were considered divisible with no particular limit in mind). There is a point of precision in each transaction that is useless because such small amounts of money are insignificant to humans. The more the price is multiplied the more the precision could matter. For example, when buying a million shares of stock, the buyer and seller might be interested in a tenth of a cent price difference, but it's only a choice. Everything else in business measurement and choice is similarly divisible to the degree that the parties are interested. For example, financial reports may be reported annually, quarterly, or monthly. Some business managers run cash-flow reports more than once per day.

Although time may be infinitely divisible, data on securities prices are reported at discrete times. For example, if one looks at records of stock prices in the 1920s, one may find the prices at the end of each day, but perhaps not at three-hundredths of a second after 12:47 PM. A new method, however, theoretically, could report at double the rate, which would not prevent further increases of velocity of reporting. Perhaps paradoxically, technical mathematics applied to financial markets is often simpler if infinitely divisible time is used as an approximation. Even in those cases, a precision is chosen with which to work, and measurements are rounded to that approximation. In terms of human interaction, money and time are divisible, but only to the point where further division is not of value, which point cannot be determined exactly.

In order theory

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To say that the field of rational numbers is infinitely divisible (i.e. order theoretically dense) means that between any two rational numbers there is another rational number. By contrast, the ring of integers is not infinitely divisible.

Infinite divisibility does not imply gaplessness: the rationals do not enjoy the least upper bound property. That means that if one were to partition the rationals into two non-empty sets A and B where A contains all rationals less than some irrational number (π, say) and B all rationals greater than it, then A has no largest member and B has no smallest member. The field of real numbers, by contrast, is both infinitely divisible and gapless. Any linearly ordered set that is infinitely divisible and gapless, and has more than one member, is uncountably infinite. For a proof, see Cantor's first uncountability proof. Infinite divisibility alone implies infiniteness but not uncountability, as the rational numbers exemplify.

In probability distributions

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To say that a probability distribution F on the real line is infinitely divisible means that if X is any random variable whose distribution is F, then for every positive integer n there exist n independent identically distributed random variables X1, ..., Xn whose sum is equal in distribution to X (those n other random variables do not usually have the same probability distribution as X).

The Poisson distribution, the stuttering Poisson distribution,[citation needed] the negative binomial distribution, and the Gamma distribution are examples of infinitely divisible distributions — as are the normal distribution, Cauchy distribution and all other members of the stable distribution family. The skew-normal distribution is an example of a non-infinitely divisible distribution. (See Domínguez-Molina and Rocha-Arteaga (2007).)

Every infinitely divisible probability distribution corresponds in a natural way to a Lévy process, i.e., a stochastic process { Xt : t ≥ 0 } with stationary independent increments (stationary means that for s < t, the probability distribution of XtXs depends only on ts; independent increments means that that difference is independent of the corresponding difference on any interval not overlapping with [s, t], and similarly for any finite number of intervals).

This concept of infinite divisibility of probability distributions was introduced in 1929 by Bruno de Finetti.

See also

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References

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from Grokipedia
Infinite divisibility refers to the property of certain mathematical or physical entities, such as continua or probability distributions, that allows them to be subdivided into smaller components indefinitely without terminating in indivisible units. In philosophy, this concept has roots in ancient debates over the structure of and space, where it posits that magnitudes like lines or volumes can be partitioned endlessly, contrasting with atomistic views that assume minimal particles. Philosophically, infinite divisibility emerged prominently in Zeno of Elea's paradoxes around the 5th century BCE, which used the idea to argue against motion and plurality by supposing that traversing a distance requires completing an infinite number of divisions in finite time, leading to contradictions. Aristotle responded by distinguishing potential infinity—where division can proceed indefinitely as a process—from actual infinity, asserting that magnitudes are infinitely divisible only potentially, preserving the coherence of continuous wholes like lines or times without composed infinities. This framework influenced later thinkers; for instance, Leibniz embraced actual infinite division of matter, viewing it as a plenum filled with an endless hierarchy of parts reflecting the world's perfection, while rejecting mathematical infinities as fictions useful for analysis but not ontology. Debates persisted into the modern era, with Hume critiquing infinite divisibility of space as incompatible with empirical perceptions of minimal sensible parts, though he ultimately reconciled it through abstract reasoning on ideas. In , infinite divisibility finds precise formulation in , where the real line is infinitely divisible due to the density of , ensuring that between any two reals lies another, allowing endless subdivision. More prominently, in , a on Rd\mathbb{R}^d is infinitely divisible if for every positive integer nn, it equals the nn-fold of some , enabling representation as limits of compound Poisson distributions via the Lévy–Khintchine formula. This property underpins Lévy processes, including and Poisson processes, and characterizes distributions essential in modeling phenomena like financial returns or particle displacements. Key examples include the normal and gamma distributions, whose infinite divisibility facilitates theoretical extensions in stochastic analysis.

Overview

Definition

Infinite divisibility refers to the property of an entity—such as , time, , or mathematical continua—that allows it to be divided into arbitrarily small parts indefinitely, without reaching a minimal indivisible unit. This notion is central to the concept of a continuum, where the whole maintains its unity despite concealing a potentially infinite plurality of divisible components. In essence, it describes structures or substances that lack inherent atomic boundaries, enabling perpetual subdivision in theory. Unlike finite divisibility, which terminates at discrete, indivisible units (such as atoms in certain philosophical or physical models), infinite divisibility permits endless partitioning without a foundational limit. Finite approaches assume a composition from basic building blocks that cannot be further broken down, whereas infinite divisibility rejects such discreteness, emphasizing continuity over granularity. Common examples span disciplines: and time are regarded as infinitely divisible continua in , comprising infinitely many points or instants within any finite extent. , in philosophical continuum theories, shares this trait, allowing theoretical division without atomic remnants. Mathematical exemplars include , divisible into smaller intervals ad infinitum, and even money in economic models, treated as continuously apportionable for precise valuation akin to real quantities. The idea is briefly illustrated in , which highlight challenges in traversing infinitely divisible distances.

Historical Context

The concept of infinite divisibility originated in around the 5th century BCE, where pre-Socratic philosophers debated the nature of matter and the continuum. Pre-Socratic philosophers such as and advocated continuously divisible substances for matter, while and proposed indivisible atoms, laying early groundwork for the tension between discrete and continuous views of the universe. A pivotal milestone came with around 450 BCE, whose paradoxes challenged the infinite divisibility of space and motion, arguing that continuous division leads to logical absurdities in traversing distances. , in the 4th century BCE, resolved some of these issues by distinguishing potential infinity—where division can proceed indefinitely without completion—from actual infinity, which he deemed impossible for physical continua, influencing Western thought for millennia. During the medieval and periods, scholastic philosophers continued these debates on the divisibility of continua. in the 13th century rejected actual infinity, aligning with to argue that continua are infinitely divisible in potential but not composed of indivisibles. Figures like and in the 14th century further refuted using geometrical arguments, emphasizing the density of continua without minimal parts. By the , and in the 15th–16th centuries began embracing actual infinities, proposing an infinite universe that extended divisibility concepts cosmologically. The Enlightenment in the 17th–18th centuries shifted focus toward space and time, with viewing both as relational and infinitely divisible, contrasting Isaac Newton's absolute framework that incorporated infinitesimally small increments in his . In the 19th and 20th centuries, formalized these ideas through Georg Cantor's , which handled actual infinities and the dense divisibility of real numbers, alongside developments in . Paul Lévy's work in the 1930s characterized infinitely divisible probability distributions, extending the concept to processes. In the 21st century, discussions persist in theories like , which posit quanta at the Planck scale, challenging classical infinite divisibility. Similarly, digital economics since Bitcoin's introduction in highlights finite but highly divisible units like satoshis, prompting debates on practical limits to divisibility in virtual assets.

Mathematics

Order Theory

In order theory, infinite divisibility within partially ordered sets (posets) refers to structural properties allowing for unbounded subdivision in the order relation. Specifically, in a poset equipped with a divisibility order, an element xx is infinitely divisible if it admits infinitely many distinct divisors below it, corresponding to an infinite collection of elements y1,y2,y_1, y_2, \dots such that each yixy_i \leq x and the divisors form a or of unbounded length. Alternatively, the poset itself exhibits infinite divisibility if it permits infinite descending s without minimal elements, meaning there exist sequences x1>x2>x3>x_1 > x_2 > x_3 > \dots with no least element, reflecting a lack of foundational atoms in the order structure. A key example contrasting finite and infinite divisibility is the poset of natural numbers under the divisibility order (N,)(\mathbb{N}, \mid), where aba \leq b if aa divides bb. This poset is finitely generated in the sense that every descending chain terminates due to the well-founded nature of the order—numbers decrease in magnitude, ensuring no infinite descending chains and thus no infinitely divisible elements. In contrast, the positive rational numbers under the usual order (Q+,<)(\mathbb{Q}^+, <) form a dense divisible , where between any two elements there exists another, enabling the construction of infinite descending chains (e.g., 1>1/2>1/3>1 > 1/2 > 1/3 > \dots) without minimal elements, embodying infinite divisibility through its . Divisible abelian groups provide a algebraic perspective intertwined with , particularly when groups are equipped with compatible orders. An GG is divisible if for every element gGg \in G and every positive nn, there exists hGh \in G such that nh=gn h = g, ensuring every element is "divisible" by any ; the infinite aspect arises from the absence of torsion in the torsion-free case, allowing repeated division indefinitely without reaching zero. The rational numbers Q\mathbb{Q} under exemplify this, as they form a torsion-free that, when ordered, yields a dense linear order supporting infinite descending chains. Properties of infinite divisibility in these structures highlight distinctions between dense orders and atomic lattices. Dense orders like (Q,<)(\mathbb{Q}, <) lack atoms (indivisible minimal elements above the bottom) and admit no finite basis for their divisibility, as subdivision can continue arbitrarily; atomic lattices, such as the divisibility lattice on integers, possess atoms (e.g., primes) and finite descending chains, limiting divisibility to bounded depths. This contrast underscores that infinite divisibility precludes finite generation, requiring infinite structural complexity. A fundamental result in this area is the structure theorem for divisible abelian groups: every divisible abelian group is isomorphic to a direct sum of copies of the additive group of rationals Q\mathbb{Q} (the torsion-free part) and Prüfer pp-groups Z(p)\mathbb{Z}(p^\infty) for various primes pp (the torsion part), as established by Baer's theorem in the 1930s. This decomposition reveals the infinite nature of divisibility, as both Q\mathbb{Q} and Z(p)\mathbb{Z}(p^\infty) support unending division—Q\mathbb{Q} through rational multiples and Z(p)\mathbb{Z}(p^\infty) through pp-power roots in its cyclic quotients.

Real Analysis

In real analysis, the real line R\mathbb{R} exhibits infinite divisibility in the sense that every non-degenerate interval (a,b)(a, b) with a<ba < b contains subintervals of arbitrary positive length less than bab - a. This property follows from the density of R\mathbb{R} in itself and its connectedness as a topological space, allowing repeated subdivision without encountering indivisible units or gaps. The completeness of R\mathbb{R}, established via Dedekind's construction using cuts, underpins this divisibility by ensuring the absence of gaps in the continuum. A partitions the rationals Q\mathbb{Q} into two non-empty classes AA and BB such that every element of AA is less than every element of BB, and AA has no greatest element; each such cut corresponds to a unique real number, filling potential voids left by Q\mathbb{Q}. This completeness permits endless bisection, as illustrated by iterative application of the midpoint theorem: for any interval (a,b)(a, b), the midpoint (a+b)/2(a + b)/2 lies within it, and the process can continue indefinitely, generating nested subintervals converging to any point in (a,b)(a, b). In measure theory, the Lebesgue measure λ\lambda on R\mathbb{R} is infinitely divisible, meaning that for any measurable set ERE \subset \mathbb{R} with λ(E)>0\lambda(E) > 0, EE can be partitioned into measurable subsets with any prescribed positive measure up to λ(E)\lambda(E). This stems from λ\lambda being a non-atomic (or diffuse) measure: no set of positive measure is an atom, allowing division into subsets AEA \subset E such that λ(A)=tλ(E)\lambda(A) = t \cdot \lambda(E) for any t[0,1]t \in [0, 1], as guaranteed by the Lyapunov convexity theorem for finite-measure spaces. For infinite-measure sets like R\mathbb{R} itself, local finiteness ensures similar partitions on bounded subsets of positive measure. In contrast, the rational numbers Q\mathbb{Q}, while dense in R\mathbb{R} and countable, lack completeness, exhibiting gaps at irrational points that hinder true infinite subdivision. For instance, the Dedekind cut defining 2\sqrt{2}
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