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Diffeology
Diffeology
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In mathematics, a diffeology on a set generalizes the concept of a smooth atlas of a differentiable manifold, by declaring only what constitutes the "smooth parametrizations" into the set. A diffeological space is a set equipped with a diffeology. Many of the standard tools of differential geometry extend to diffeological spaces, which beyond manifolds include arbitrary quotients of manifolds, arbitrary subsets of manifolds, and spaces of mappings between manifolds.

Introduction

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Calculus on "smooth spaces"

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The differential calculus on , or, more generally, on finite dimensional vector spaces, is one of the most impactful successes of modern mathematics. Fundamental to its basic definitions and theorems is the linear structure of the underlying space.[1][2]

The field of differential geometry establishes and studies the extension of the classical differential calculus to non-linear spaces. This extension is made possible by the definition of a smooth manifold, which is also the starting point for diffeological spaces.

A smooth -dimensional manifold is a set equipped with a maximal smooth atlas, which consists of injective functions, called charts, of the form , where is an open subset of , satisfying some mutual-compatibility relations. The charts of a manifold perform two distinct functions, which are often syncretized:[3][4][5]

  • They dictate the local structure of the manifold. The chart identifies its image in with its domain . This is convenient because the latter is simply an open subset of a Euclidean space.
  • They define the class of smooth maps between manifolds. These are the maps to which the differential calculus extends. In particular, the charts determine smooth functions (smooth maps ), smooth curves (smooth maps ), smooth homotopies (smooth maps ), etc.

A diffeology generalizes the structure of a smooth manifold by abandoning the first requirement for an atlas, namely that the charts give a local model of the space, while retaining the ability to discuss smooth maps into the space.[6][7][8]

Informal definition

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A diffeological space is a set equipped with a diffeology: a collection of mapswhose members are called plots, that satisfies some axioms. The plots are not required to be injective, and can (indeed, must) have as domains the open subsets of arbitrary Euclidean spaces.

A smooth manifold can be viewed as a diffeological space which is locally diffeomorphic to . In general, while not giving local models for the space, the axioms of a diffeology still ensure that the plots induce a coherent notion of smooth functions, smooth curves, smooth homotopies, etc. Diffeology is therefore suitable to treat objects more general than manifolds.[6][7][8]

Motivating example

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Let and be smooth manifolds. A smooth homotopy of maps is a smooth map . For each , the map is smooth, and the intuition behind a smooth homotopy is that it is a smooth curve into the space of smooth functions connecting, say, and . But is not a finite-dimensional smooth manifold, so formally we cannot yet speak of smooth curves into it.

On the other hand, the collection of maps is a diffeology on . With this structure, the smooth curves (a notion which is now rigorously defined) correspond precisely to the smooth homotopies.[6][7][8]

History

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The concept of diffeology was first introduced by Jean-Marie Souriau in the 1980s under the name espace différentiel.[9][10] Souriau's motivating application for diffeology was to uniformly handle the infinite-dimensional groups arising from his work in geometric quantization. Thus the notion of diffeological group preceded the more general concept of a diffeological space. Souriau's diffeological program was taken up by his students, particularly Paul Donato[11] and Patrick Iglesias-Zemmour,[12] who completed early pioneering work in the field.

A structure similar to diffeology was introduced by Kuo-Tsaï Chen (陳國才, Chen Guocai) in the 1970s, in order to formalize certain computations with path integrals. Chen's definition used convex sets instead of open sets for the domains of the plots.[13] The similarity between diffeological and "Chen" structures can be made precise by viewing both as concrete sheaves over the appropriate concrete site.[14]

Formal definition

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A diffeology on a set consists of a collection of maps, called plots or parametrizations, from open subsets of (for all ) to such that the following axioms hold:

  • Covering axiom: every constant map is a plot.
  • Locality axiom: for a given map , if every point in has a neighborhood such that is a plot, then itself is a plot.
  • Smooth compatibility axiom: if is a plot, and is a smooth function from an open subset of some into the domain of , then the composite is a plot.

Note that the domains of different plots can be subsets of for different values of ; in particular, any diffeology contains the elements of its underlying set as the plots with . A set together with a diffeology is called a diffeological space.

More abstractly, a diffeological space is a concrete sheaf on the site of open subsets of , for all , and open covers.[14]

Morphisms

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A map between diffeological spaces is called smooth if and only if its composite with any plot of the first space is a plot of the second space. It is called a diffeomorphism if it is smooth, bijective, and its inverse is also smooth. Equipping the open subsets of Euclidean spaces with their standard diffeology (as defined in the next section), the plots into a diffeological space are precisely the smooth maps from to .

Diffeological spaces constitute the objects of a category, denoted by , whose morphisms are smooth maps. The category is closed under many categorical operations: for instance, it is Cartesian closed, complete and cocomplete, and more generally it is a quasitopos.[14]

D-topology

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Any diffeological space is a topological space when equipped with the D-topology:[12] the final topology such that all plots are continuous (with respect to the Euclidean topology on ).

In other words, a subset is open if and only if is open for any plot on . Actually, the D-topology is completely determined by smooth curves, i.e. a subset is open if and only if is open for any smooth map .[15] The D-topology is automatically locally path-connected[16]

A smooth map between diffeological spaces is automatically continuous between their D-topologies.[6] Therefore we have the functor , from the category of diffeological spaces to the category of topological spaces, which assigns to a diffeological space its D-topology. This functor realizes as a concrete category over .

Additional structures

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A Cartan-De Rham calculus can be developed in the framework of diffeologies, as well as a suitable adaptation of the notions of fiber bundles, homotopy, etc.[6] However, there is not a canonical definition of tangent spaces and tangent bundles for diffeological spaces.[17]

Examples

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First examples

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Any set carries at least two diffeologies:

  • the coarse (or trivial, or indiscrete) diffeology, consisting of every map into the set. This is the largest possible diffeology. The corresponding D-topology is the trivial topology.
  • the discrete (or fine) diffeology, consisting of the locally constant maps into the set. This is the smallest possible diffeology. The corresponding D-topology is the discrete topology.

Any topological space can be endowed with the continuous diffeology, whose plots are the continuous maps.

The Euclidean space admits several diffeologies beyond those listed above.

  • The standard diffeology on consists of those maps which are smooth in the usual sense of multivariable calculus.
  • The wire (or spaghetti) diffeology on is the diffeology whose plots factor locally through . More precisely, a map is a plot if and only if for every there is an open neighbourhood of such that for two smooth functions and . This diffeology does not coincide with the standard diffeology on when : for instance, the identity is not a plot for the wire diffeology.[6]
  • The previous example can be enlarged to diffeologies whose plots factor locally through , yielding the rank--restricted diffeology on a smooth manifold : a map is a plot if and only if it is smooth and the rank of its differential is less than or equal than . For one recovers the wire diffeology.[18]

Relation to other smooth spaces

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Diffeological spaces generalize manifolds, but they are far from the only mathematical objects to do so. For instance manifolds with corners, orbifolds, and infinite-dimensional Fréchet manifolds are all well-established alternatives. This subsection makes precise the extent to which these spaces are diffeological.

We view as a concrete category over the category of topological spaces via the D-topology functor . If is another concrete category over , we say that a functor is an embedding (of concrete categories) if it is injective on objects and faithful, and . To specify an embedding, we need only describe it on objects; it is necessarily the identity map on arrows.

We will say that a diffeological space is locally modeled by a collection of diffeological spaces if around every point , there is a D-open neighbourhood , a D-open subset of some , and a diffeological diffeomorphism .[6][19]

Manifolds

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The category of finite-dimensional smooth manifolds (allowing those with connected components of different dimensions) fully embeds into . The embedding assigns to a smooth manifold the canonical diffeologyIn particular, a diffeologically smooth map between manifolds is smooth in the usual sense, and the D-topology of is the original topology of . The essential image of this embedding consists of those diffeological spaces that are locally modeled by the collection , and whose D-topology is Hausdorff and second-countable.[6]

Manifolds with boundary or corners

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The category of finite-dimensional smooth manifolds with boundary (allowing those with connected components of different dimensions) similarly fully embeds into . The embedding is defined identically to the smooth case, except "smooth in the usual sense" refers to the standard definition of smooth maps between manifolds with boundary. The essential image of this embedding consists of those diffeological spaces that are locally modeled by the collection , and whose D-topology is Hausdorff and second-countable. The same can be done in more generality for manifolds with corners, using the collection .[20]

Fréchet and Banach manifolds

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The category of Fréchet manifolds similarly fully embeds into . Once again, the embedding is defined identically to the smooth case, except "smooth in the usual sense" refers to the standard definition of smooth maps between Fréchet spaces. The essential image of this embedding consists of those diffeological spaces that are locally modeled by the collection , and whose D-topology is Hausdorff.

The embedding restricts to one of the category of Banach manifolds. Historically, the case of Banach manifolds was proved first, by Hain,[21] and the case of Fréchet manifolds was treated later, by Losik.[22][23] The category of manifolds modeled on convenient vector spaces also similarly embeds into .[24][25]

Orbifolds

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A (classical) orbifold is a space that is locally modeled by quotients of the form , where is a finite subgroup of linear transformations. On the other hand, each model is naturally a diffeological space (with the quotient diffeology discussed below), and therefore the orbifold charts generate a diffeology on . This diffeology is uniquely determined by the orbifold structure of .

Conversely, a diffeological space that is locally modeled by the collection (and with Hausdorff D-topology) carries a classical orbifold structure that induces the original diffeology, wherein the local diffeomorphisms are the orbifold charts. Such a space is called a diffeological orbifold.[26]

Whereas diffeological orbifolds automatically have a notion of smooth map between them (namely diffeologically smooth maps in ), the notion of a smooth map between classical orbifolds is not standardized.

If orbifolds are viewed as differentiable stacks presented by étale proper Lie groupoids, then there is a functor from the underlying 1-category of orbifolds, and equivalent maps-of-stacks between them, to . Its essential image consists of diffeological orbifolds, but the functor is neither faithful nor full.[27]

Constructions

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Intersections

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If a set is given two different diffeologies, their intersection is a diffeology on , called the intersection diffeology, which is finer than both starting diffeologies. The D-topology of the intersection diffeology is finer than the intersection of the D-topologies of the original diffeologies.

Products

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If and are diffeological spaces, then the product diffeology on the Cartesian product is the diffeology generated by all products of plots of and of . Precisely, a map necessarily has the form for maps and . The map is a plot in the product diffeology if and only if and are plots of and , respectively. This generalizes to products of arbitrary collections of spaces.

The D-topology of is the coarsest delta-generated topology containing the product topology of the D-topologies of and ; it is equal to the product topology when or is locally compact, but may be finer in general.[15]

Pullbacks

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Given a map from a set to a diffeological space , the pullback diffeology on consists of those maps such that the composition is a plot of . In other words, the pullback diffeology is the smallest diffeology on making smooth.

If is a subset of the diffeological space , then the subspace diffeology on is the pullback diffeology induced by the inclusion . In this case, the D-topology of is equal to the subspace topology of the D-topology of if is open, but may be finer in general.

Pushforwards

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Given a map from diffeological space to a set , the pushforward diffeology on is the diffeology generated by the compositions , for plots of . In other words, the pushforward diffeology is the smallest diffeology on making smooth.

If is a diffeological space and is an equivalence relation on , then the quotient diffeology on the quotient set is the pushforward diffeology induced by the quotient map . The D-topology on is the quotient topology of the D-topology of . Note that this topology may be trivial without the diffeology being trivial.

Quotients often give rise to non-manifold diffeologies. For example, the set of real numbers is a smooth manifold. The quotient , for some irrational , called the irrational torus, is a diffeological space diffeomorphic to the quotient of the regular 2-torus by a line of slope . It has a non-trivial diffeology, although its D-topology is the trivial topology.[28]

Functional diffeologies

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The functional diffeology on the set of smooth maps between two diffeological spaces and is the diffeology whose plots are the maps such thatis smooth with respect to the product diffeology of . When and are manifolds, the D-topology of is the smallest locally path-connected topology containing the Whitney topology.[15]

Taking the subspace diffeology of a functional diffeology, one can define diffeologies on the space of sections of a fibre bundle, or the space of bisections of a Lie groupoid, etc.

If is a compact smooth manifold, and is a smooth fiber bundle over , then the space of smooth sections of the bundle is frequently equipped with the structure of a Fréchet manifold.[29] Upon embedding this Fréchet manifold into the category of diffeological spaces, the resulting diffeology coincides with the subspace diffeology that inherits from the functional diffeology on .[30]

Distinguished maps between diffeological spaces

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Analogous to the notions of submersions and immersions between manifolds, there are two special classes of morphisms between diffeological spaces. A subduction is a surjective function between diffeological spaces such that the diffeology of is the pushforward of the diffeology of . Similarly, an induction is an injective function between diffeological spaces such that the diffeology of is the pullback of the diffeology of . Subductions and inductions are automatically smooth.

It is instructive to consider the case where and are smooth manifolds.

  • Every surjective submersion is a subduction.
  • A subduction need not be a surjective submersion. One example is
  • An injective immersion need not be an induction. One example is the parametrization of the "figure-eight,"

  • An induction need not be an injective immersion. One example is the "semi-cubic,"[31][32]

In the category of diffeological spaces, subductions are precisely the strong epimorphisms, and inductions are precisely the strong monomorphisms.[18] A map that is both a subduction and induction is a diffeomorphism.

References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Diffeology is a mathematical framework in that generalizes the concept of on arbitrary sets, extending traditional by defining via plots— from of —rather than requiring an of coordinate charts. Introduced by French mathematician Jean-Marie Souriau in the 1980s under the original name "espace différentiel," it provides a flexible approach to handle spaces that do not fit the standard paradigm, such as those with or infinite-dimensional structures. This framework, rigorously formalized through a minimal set of axioms, allows for the study of on diffeological spaces without the constraints of imposed by . Key developments were advanced by Patrick Iglesias-Zemmour, whose work, including the seminal book Diffeology published by the , has established it as a powerful tool for exploring concepts like diffeological groups, functional diffeology, and integration on non-standard spaces. Diffeology distinguishes itself by its applicability beyond , enabling rigorous treatment of objects in , , and , where traditional methods falter—for instance, in modeling configuration spaces of physical systems or classifying spaces in . It supports the definition of , , and differential forms in a diffeological context, fostering connections to Lie groupoids and , and has been influential in modern research on generalized geometry.

Definition and Fundamentals

Definition of Diffeology

A diffeology on a set XX is defined as a subset DParams(X)\mathcal{D} \subset \mathrm{Params}(X), where Params(X)\mathrm{Params}(X) denotes the collection of all parametrizations from Euclidean domains into XX, and the elements of D\mathcal{D} are called plots. A parametrization is a map P:UXP: U \to X, where UU is an open subset of some Rn\mathbb{R}^n for nNn \in \mathbb{N}, with no requirements such as injectivity imposed on PP. The diffeology D\mathcal{D} must satisfy three core axioms to ensure a consistent notion of smoothness: the covering axiom, the locality axiom, and the smooth compatibility axiom. A map ϕ:UX\phi: U \to X is a D\mathcal{D}-plot if it belongs to D\mathcal{D}, thereby satisfying these axioms by construction. The covering axiom states that D\mathcal{D} contains all constant parametrizations. Specifically, for any Euclidean domain UU and any xXx \in X, the constant map P:UXP: U \to X defined by P(r)=xP(r) = x for all rUr \in U must be in D\mathcal{D}. This axiom establishes a , ensuring that single points in XX can be and providing a foundation for more complex plots, as are inherently smooth in any . The locality axiom requires that is a local property. Formally, if P:UXP: U \to X is a such that for every rUr \in U, there exists an VUV \subset U of rr with PVDP|_V \in \mathcal{D}, then PDP \in \mathcal{D}. This means that a qualifies as a plot if it can be decomposed into local pieces that are themselves plots, reflecting the principle that global smoothness arises from without needing a predefined on XX. Consequently, restrictions of plots to of their domains also remain plots, preserving the plot status under domain subsetting. The smooth compatibility axiom ensures closure under reparametrization. It stipulates that for any plot P:UXP: U \to X in D\mathcal{D} and any F:VUF: V \to U between Euclidean domains (i.e., ), the composite map PF:VXP \circ F: V \to X is also in D\mathcal{D}. This axiom guarantees that the diffeology is invariant under smooth changes of coordinates in the , allowing compositions that maintain the and aligning diffeology with the compositional nature of smoothness in . A diffeological space is simply a equipped with such a diffeology.

Diffeological Spaces

A diffeological space is formally defined as a set XX equipped with a diffeology D\mathcal{D} on XX, where the diffeology specifies a collection of smooth parametrizations, known as plots, that endow the set with a generalized smooth structure. This framework, introduced by Jean-Marie Souriau and developed by Patrick Iglesias-Zemmour, extends beyond by allowing to be defined intrinsically through these plots rather than requiring a . One key intrinsic property of diffeological spaces is that is determined internally via the plots, which enables the construction of on spaces that may be , , or otherwise incompatible with . Plots serve as the fundamental building blocks, providing a flexible way to define local smoothness without imposing global topological constraints. This internal definition preserves essential while broadening applicability to or pathological sets. In diffeology, are defined at points of a diffeological space either through tangent plots, which are derivations along smooth curves, or via the acting on germs of . These constructions yield a tangent space [TxX](/page/Tangentspace)[T_x X](/page/Tangent_space) at each point xXx \in X that behaves like a vector space, facilitating the study of velocities and directions in a manner analogous to . Diffeological spaces form a category denoted Diff, where the objects are diffeological spaces and the are smooth maps compatible with the respective diffeologies. This category is particularly well-behaved, being complete, cocomplete, and , which supports advanced constructions like limits and in a smooth context.

Plots and Smooth Maps

In diffeology, the smooth structure on a set XX is defined through a collection of maps known as plots. A plot of a diffeological space (X,D)(X, \mathcal{D}) is a map ϕ:UX\phi: U \to X, where UU is an open subset of some Euclidean space Rn\mathbb{R}^n for n0n \geq 0, and ϕ\phi belongs to the diffeology D\mathcal{D}, which is a specified family of such maps satisfying three axioms: coverage (every point of XX is in the image of some plot), locality (a map is a plot if it is locally a plot), and smooth compatibility (the composition of a plot with a smooth map from another Euclidean domain into its domain is again a plot). These plots serve as the basic parametrizations that encode the notion of smoothness on XX, generalizing the local charts used in classical differentiable manifolds by allowing for more flexible and global descriptions, particularly for spaces that are not Hausdorff or of varying dimension. Smooth maps between diffeological spaces are defined in terms of their compatibility with plots, providing a natural notion of in the category of diffeological spaces. Specifically, given diffeological spaces (X,DX)(X, \mathcal{D}_X) and (Y,DY)(Y, \mathcal{D}_Y), a map f:XYf: X \to Y is smooth if, for every plot ϕ:UX\phi: U \to X in DX\mathcal{D}_X, the composition fϕ:UYf \circ \phi: U \to Y is a plot in DY\mathcal{D}_Y. This condition can be expressed formally as: ϕDX(U),fϕDY(U),\forall \, \phi \in \mathcal{D}_X(U), \quad f \circ \phi \in \mathcal{D}_Y(U), where URnU \subseteq \mathbb{R}^n is open. The set of all such smooth maps from XX to YY is denoted C(X,Y)C^\infty(X, Y) and inherits a natural diffeological structure, making the category {Diffeology}\{ \text{Diffeology} \} Cartesian closed. A key concept underlying this definition is the lifting property for , which ensures that is preserved under with parametrizations from . This property means that to verify the smoothness of ff, it suffices to check that plots into XX "lift" through ff to become plots into YY, thereby maintaining compatibility with the on Euclidean domains and extending the to arbitrary diffeological spaces. For instance, on , this reduces to the usual definition of , as plots correspond to ordinary smooth maps from in .

Historical Development

Origins and Introduction

Diffeology was introduced by French mathematician Jean-Marie Souriau in the early 1980s as a framework to generalize beyond traditional , initially under the name "difféologies" or "espace différentiel." This concept first appeared in Souriau's 1980 paper "Groupes Différentiels," published in the Lecture Notes in Mathematics, volume 836, where it was presented as a set of axioms for defining on groups, particularly to address of diffeomorphisms. The term "espace différentiel" emerged shortly thereafter, formalized in Souriau's 1983 publication "Groupes différentiels et physique mathématique," marking the shift toward a broader theory applicable to rather than just groups. The primary motivation for diffeology arose from challenges in and , where traditional struggled to provide on , such as quotients by group actions that result in or . Souriau sought to handle these issues, exemplified by the need to study irrational tori—quotients of the by dense subgroups that lack non-constant smooth functions under —while maintaining compatibility with physical applications like with . This framework allowed for a unified treatment of such non-manifold spaces in physics and geometry, enabling the definition of via plots that could accommodate without requiring a . Souriau's initial formulations were outlined in his 1980s lectures and papers on , where diffeology provided tools for working with and in . By separating general axioms for differential spaces from group-specific ones, as refined in collaborations during this period, diffeology established a flexible category stable under quotients and products, directly addressing the limitations of for these motivating problems.

Key Contributors and Publications

The foundational concept of diffeology traces its roots to the work of Jean-Marie Souriau, who introduced the notion of espace différentiel in the 1980s as a framework for handling on non-standard spaces, particularly in the context of and . Souriau's seminal contributions include the 1980 paper "Groupes différentiels" in Lecture Notes in Mathematics, which laid the groundwork for defining via plots, and subsequent works such as those published in 1984 that expanded on differential groups. Patrick Iglesias-Zemmour played a pivotal role in the development and systematization of diffeology during the 1990s and 2000s, transforming Souriau's initial ideas into a comprehensive theory applicable to a wide range of singular and quotient spaces. The term "diffeology" was suggested by W.T. van Est in the mid-1980s during the defense of Paul Donato's thesis, as a replacement for "différentiel," building on Souriau's foundational ideas, with Iglesias-Zemmour emphasizing its categorical and aspects beyond traditional . Iglesias-Zemmour's key publications include the 2010 monograph The Moment Maps in Diffeology, which explores and within the diffeological setting, and the influential 2013 textbook Diffeology published by the , which provides a detailed exposition of the theory's fundamentals and constructions. Other notable contributors include collaborators influenced by Souriau's efforts, though specific influences from figures like Jean-Michel Bismut remain tied to broader contexts without direct diffeological attributions in primary sources. Iglesias-Zemmour's surveys, such as "An Introduction to Diffeology" (circa , with updates in later lectures), further disseminated the theory, bridging it to and fiber bundle applications. Recent extensions of diffeology appear in preprints, including Iglesias-Zemmour's 2025 paper "Why Diffeology?", which highlights its advantages for and , and the 2025 work "Groupoids in Diffeology" by various authors, advancing the theory's structures. Additional preprints, such as "Nonstandard diffeology and generalized functions" (2024) and "Tangent spaces of diffeological spaces and their variants" (2024), explore and refinements, indicating ongoing developments in the field.

Key Properties and Structures

Categorical Aspects

The category of diffeological spaces, denoted Diff, has as objects diffeological spaces and as morphisms smooth maps between them. This category is cartesian closed, meaning that for any diffeological spaces XX and YY, the [X,Y][X, Y] exists as a diffeological space equipped with the functional diffeology, and the evaluation map [X,Y]×XY[X, Y] \times X \to Y is smooth. The cartesian closed structure arises naturally from the functional diffeology on the set of smooth maps, which generates plots as compositions of smooth maps from open subsets of . There exists a U: \Diff \to \Set that sends a diffeological space to its underlying set and a smooth map to its underlying function, preserving all limits and colimits since diffeologies are defined set-theoretically via plots. Additionally, there is a from the category of smooth manifolds into Diff, manifolds as diffeological spaces with their standard diffeology induced by . This inclusion preserves the on manifolds but extends it to a broader categorical framework. Diff is both complete and cocomplete, allowing the construction of all small limits and colimits within the category. For products, the product diffeology on X×YX \times Y for diffeological spaces XX and YY is the finest diffeology making the projections πX:X×YX\pi_X: X \times Y \to X and πY:X×YY\pi_Y: X \times Y \to Y smooth, generated by plots of the form p=(p1,p2):UX×Yp = (p_1, p_2): U \to X \times Y where p1:UXp_1: U \to X and p2:UYp_2: U \to Y are plots. Coproducts in Diff are disjoint unions equipped with the disjoint union diffeology, where a plot into the coproduct is a plot into one factor composed with the inclusion. Pullbacks exist and are computed via the pullback in sets with the induced diffeology generated by plots that are pullbacks of plots in the defining diagram. These constructions ensure that limits and colimits in Diff align with those in the category of sets under the forgetful functor, facilitating categorical operations on diffeological spaces. Research into , such as of diffeological spaces, remains an active area, building on the foundational nature of Diff to explore enhancements.

Examples of Diffeological Spaces

Diffeological spaces encompass a wide range of mathematical objects, starting with classical examples that align with traditional . Any equipped with its standard diffeology serves as a fundamental example, where the plots are precisely the smooth maps from of into the manifold. Similarly, Euclidean spaces for any n0n \geq 0 form diffeological spaces with the standard diffeology, in which a plot is a from an in Rm\mathbb{R}^m to Rn\mathbb{R}^n. Beyond these, diffeology accommodates non-manifold spaces that defy . , such as the orbit space of a on a diffeological space, provide key non-manifold examples, where the diffeology is induced by the . , which are , can be endowed with the fine diffeology, making them diffeological spaces that extend finite-dimensional concepts to infinite dimensions while preserving . A specific and influential example is the space of probability measures on a given diffeological space, often denoted P(X)\mathcal{P}(X), equipped with a diffeology generated by plots that are maps ϕ:UP(X)\phi: U \to \mathcal{P}(X) such that for every ff on XX, the map uXfdϕ(u)u \mapsto \int_X f \, d\phi(u) is on UU. This construction is particularly useful in contexts requiring on spaces of measures. The Hawaiian earring, a singular consisting of infinitely many circles of decreasing radii joined at a point, can also be formalized as a diffeological space, allowing the study of its despite its non-manifold nature.

Subspaces, Quotients, and Products

In diffeological spaces, the subspace diffeology on a subset YXY \subseteq X of a diffeological space (X,DX)(X, \mathcal{D}_X) is induced by restricting the plots of XX to those whose images lie entirely within YY. Specifically, a map p:UYp: U \to Y, where U[Rn](/page/Euclideanspace)U \subseteq [\mathbb{R}^n](/page/Euclidean_space) is open, is a plot in the subspace diffeology if the composition ip:UXi \circ p: U \to X is a plot in DX\mathcal{D}_X, where i:YXi: Y \to X is the , ensuring the inclusion map i:YXi: Y \to X is smooth. This construction preserves the inherited from XX, making YY a diffeological space in its own right. For quotients, given a diffeological space XX and an \sim on XX, the X/X / \sim is equipped with the quotient diffeology, where a map p:UX/p: U \to X / \sim is a plot if, for every uUu \in U, there is a neighborhood VV of uu and a plot q:VXq: V \to X such that pV=πqp|_V = \pi \circ q, with π:XX/\pi: X \to X / \sim the . This defines the final diffeology with respect to π\pi, ensuring π\pi is a subduction—a surjective smooth map—and allowing the quotient to capture the even in cases with pathologies, such as non-regular quotients where the may be trivial but the diffeology remains rich. The product diffeology on X×YX \times Y for diffeological spaces XX and YY consists of maps p:UX×Yp: U \to X \times Y such that the component maps pX:UXp_X: U \to X and pY:UYp_Y: U \to Y are plots in DX\mathcal{D}_X and DY\mathcal{D}_Y, respectively; formally, p=(pX,pY)p = (p_X, p_Y) is a plot if both components satisfy the plot conditions independently. This initial diffeology with respect to the projections πX:X×YX\pi_X: X \times Y \to X and πY:X×YY\pi_Y: X \times Y \to Y ensures the projections are subductions, supporting the exponential law for smooth maps: C(X,C(Y,Z))C(X×Y,Z)C^\infty(X, C^\infty(Y, Z)) \cong C^\infty(X \times Y, Z). These operations—subspaces, quotients, and products—preserve the categorical structure of diffeological spaces, forming a complete and cocomplete category that admits all limits and colimits, thus enabling robust constructions beyond traditional .

Applications and Extensions

In Differential Geometry

In , diffeology extends classical concepts to spaces that may not possess a , allowing for the definition of geometric objects like bundles and on or infinite-dimensional sets. This framework is particularly useful for handling or non-locally Euclidean spaces that arise in reduction procedures or as in physics. By relying on plots—smooth parametrizations from Euclidean domains—diffeology ensures that is defined intrinsically without requiring or , enabling generalizations of , , and . Vector bundles in diffeology are defined using transition plots, which are smooth maps between overlapping Euclidean domains that describe how local trivializations glue together, analogous to classical transition functions but adapted to the plot-based smoothness. This construction yields diffeological vector pseudo-bundles, which may not be locally trivial in the traditional sense but still support sections and fiberwise vector space operations. The tangent bundle of a diffeological space XX is constructed using the internal tangent spaces derived from plots, forming a diffeological vector pseudo-bundle over XX with fibers that are diffeological vector spaces, while the external tangent space uses derivations on function germs; the cotangent bundle is its dual, comprising k-forms defined via pullbacks of plots. These bundles facilitate the study of tangent spaces at points, where the tangent space TxXT_x X consists of equivalence classes of curves tangent to plots at xx. on diffeological spaces are adapted by defining a that assigns to in a way compatible with the diffeology, often via plot-lifting, where the metric on a plot P:UXP: U \to X lifts to a on UU. This approach ensures that the metric is smooth with respect to the plots and extends to , accommodating singular or non-compact spaces where classical definitions fail. For instance, on non-compact diffeological spaces, such metrics can incorporate or along strata, providing a framework for without assuming . Plot-lifting preserves the under , allowing computations of lengths and directly from . A key application of diffeology in is singular reduction in , where diffeological quotients of yield reduced phase spaces that may have singularities, unlike the smooth quotients in Marsden-Weinstein reduction. In this context, the momentum map μ:(M,ω)g\mu: (M, \omega) \to \mathfrak{g}^* for a Hamiltonian group action is treated as a smooth diffeological map, and the reduced space μ1(ξ)/Gξ\mu^{-1}(\xi)/G_\xi inherits a diffeological symplectic structure via quotient diffeology. This method handles strata of different naturally, preserving on singular strata and enabling the study of stratified symplectic spaces in . Diffeological principal bundles generalize by defining them as surjective submersions PXP \to X with a smooth right action of a diffeological Lie group GG, where local triviality is ensured along plots rather than . These bundles support connections via adapted to the diffeology, facilitating and in singular settings. Such structures are crucial for on non-manifold spaces, where the bundle's total space PP may be diffeological itself.

In Homotopy Theory

In diffeology, the of smooth maps between diffeological spaces is defined using plot homotopies, where a homotopy between two smooth maps f,g:XYf, g: X \to Y is a smooth map H:X×IYH: X \times I \to Y (with II the equipped with its standard diffeology) such that H(,0)=fH(-, 0) = f and H(,1)=gH(-, 1) = g, ensuring that the homotopy respects the plot structures of both spaces. This approach generalizes to diffeological spaces, allowing for smooth deformations that capture topological features in a differential setting. The of a diffeological space XX, denoted Π(X)\Pi(X), is constructed with points of XX as objects and fixed-end homotopy classes of paths in XX as , where paths are defined as from the II to XX, and yield the π1(X,x)\pi_1(X, x). This structure extends the classical to diffeological contexts, enabling the study of path spaces as diffeological spaces themselves and facilitating computations of like through inductive constructions on plot dimensions. Diffeology provides a smooth model for beyond traditional , particularly for singular spaces, by equipping objects like and configuration spaces with natural diffeological structures that support . For instance, the of a diffeological group GG is defined via a diffeology on the of the nerve, allowing and to be handled smoothly even when GG is infinite-dimensional. Similarly, configuration spaces of points in a manifold, such as the ordered configuration space Fk(M)F_k(M) for kk points in MM, inherit a diffeology that preserves smoothness in , aiding applications in and equivariant homotopy theory. This flexibility highlights diffeology's role in modeling homotopy types that elude manifold-based approaches.

Integration and Calculus on Diffeological Spaces

In diffeological spaces, differential forms are defined as assignments of smooth forms on the domains of plots to the plots themselves, ensuring compatibility under composition. Specifically, a kk-form ω\omega on a diffeological space XX associates to each plot P:UXP: U \to X, where URnU \subset \mathbb{R}^n is open, a smooth kk-form ω(P)\omega(P) on UU such that ω(PF)=Fω(P)\omega(P \circ F) = F^* \omega(P) for any smooth map F:VUF: V \to U from another open set VRmV \subset \mathbb{R}^m. This definition extends the classical notion on manifolds, where forms are sections of the exterior bundle, by relying on the diffeological structure of plots rather than a tangent bundle, allowing smoothness on non-manifold spaces. The alternation axiom is implicitly satisfied through the antisymmetric nature of the assigned forms on Euclidean domains. The on a diffeological space XX is formed by the Ω(X)=k0Ωk(X)\Omega^*(X) = \bigoplus_{k \geq 0} \Omega^k(X) of all differential forms, equipped with the exterior derivative d:Ωk(X)Ωk+1(X)d: \Omega^k(X) \to \Omega^{k+1}(X) defined by [dω](P)=d[ω(P)][d\omega](P) = d[\omega(P)] for each plot PP, where dd on the right is the standard exterior derivative on the domain of PP. This satisfies d2=0d^2 = 0 due to the corresponding property on , yielding ZdRk(X)=kerdZ^k_{dR}(X) = \ker d and exact forms BdRk(X)=imdB^k_{dR}(X) = \operatorname{im} d, with HdRk(X)=ZdRk(X)/BdRk(X)H^k_{dR}(X) = Z^k_{dR}(X) / B^k_{dR}(X). For plots ϕ:UX\phi: U \to X, the chain rule holds as d(ωϕ)=(dω)ϕd(\omega \circ \phi) = (d\omega) \circ \phi, mirroring the on manifolds and ensuring the complex is well-defined. When XX is a equipped with its manifold diffeology, the diffeological de Rham cohomology recovers the via a induced by the tautological map τ:ΩDR(X)Ω(X)\tau: \Omega^*_{DR}(X) \to \Omega^*(X), defined by τ(η)={ϕη}ϕD(X)\tau(\eta) = \{\phi^* \eta \}_{\phi \in D(X)} for plots ϕ\phi. Integration on diffeological spaces is defined over cubic chains, which are finite integer linear combinations of pp-cubes σC([0,1]p,X)\sigma \in C^\infty([0,1]^p, X). For a pp-form α\alpha and pp-cube σ\sigma, the integral is σα=[0,1]pα(σ)\int_\sigma \alpha = \int_{[0,1]^p} \alpha(\sigma), where α(σ)\alpha(\sigma) is the pulled-back form on [0,1]p[0,1]^p, reducible to a multiple integral 0101fσ(x)dx1dxp\int_0^1 \cdots \int_0^1 f_\sigma(x) \, dx_1 \cdots dx_p with fσ(x)=α(σ)x(e1,,ep)f_\sigma(x) = \alpha(\sigma)_x(e_1, \dots, e_p) for the standard basis eie_i. This extends linearly to chains c=nσσc = \sum n_\sigma \sigma as cα=nσσα\int_c \alpha = \sum n_\sigma \int_\sigma \alpha, providing a pushforward-like mechanism via the plots underlying the cubes. The diffeological Stokes' theorem holds: for a (p1)(p-1)-form α\alpha and pp-chain cc, cdα=cα\int_c d\alpha = \int_{\partial c} \alpha, proved by reducing to integrals on standard cubes in Rp\mathbb{R}^p. The Cartan-de Rham theorem in diffeology manifests as an between certain , particularly for quotients like of . For a (M,F)(M, \mathcal{F}), the projection p:MM/Fp: M \to M/\mathcal{F} (with quotient diffeology) induces p:Ωb(M,F)Ω(M/F)p^*: \Omega^*_b(M, \mathcal{F}) \to \Omega^*(M/\mathcal{F}), an isomorphism of complexes where Ωb(M,F)\Omega^*_b(M, \mathcal{F}) consists of base-like forms, yielding Hb(M,F)HdR(M/F)H^*_b(M, \mathcal{F}) \cong H^*_{dR}(M/\mathcal{F}). This is constructed via maps involving and , generalizing the classical theorem by relating invariant forms on the to the on the diffeological quotient. Additionally, a chain-homotopy operator K:Ωp(X)Ωp1(Paths(X))K: \Omega^p(X) \to \Omega^{p-1}(\mathrm{Paths}(X)) satisfies dK+Kd=1^0^dK + Kd = \hat{1}^* - \hat{0}^*, proving of and extending Cartan-de Rham tools like the LF(α)=iF(dα)+d(iF(α))L_F(\alpha) = i_F(d\alpha) + d(i_F(\alpha)) for slidings FF.

Comparisons and Relations

Relation to Differentiable Manifolds

Diffeological spaces generalize the notion of by providing a framework where is defined intrinsically through plots, allowing to be embedded as a special case. Every can be equipped with a canonical diffeology, where the plots are precisely the smooth maps from of into the manifold, making the category of smooth manifolds a of the category of diffeological spaces. This preserves the , as the standard diffeology on serves as the foundational model for in manifolds. Conversely, a diffeological space qualifies as a smooth nn-manifold if it is locally diffeomorphic to Rn\mathbb{R}^n at every point, meaning that around each point, there exists a neighborhood diffeomorphic to an open subset of Rn\mathbb{R}^n in the diffeological sense. This condition ensures that the diffeology is generated by a compatible smooth atlas, recovering the classical manifold structure exactly when the space satisfies the additional topological requirements of being Hausdorff and second-countable. In such cases, the diffeological smooth maps between manifolds coincide precisely with the smooth maps defined in traditional differential geometry. A key distinction arises in the flexibility of diffeology, which does not impose the required for , enabling the study of non-Hausdorff spaces like the irrational torus, obtained as a of the by a dense subgroup, which has but admits a non-trivial diffeology via pushforwards of plots. Similarly, diffeology accommodates non-second-countable spaces, such as the space of all smooth maps between two , which typically fails these topological constraints. These features allow diffeology to extend to pathological or without the rigid topological constraints of .

Relation to Other Geometric Theories

Diffeology provides a more permissive framework than the differential spaces introduced by Kryszewski and Siciak, which rely on derivations or generated by maps from the space to , whereas diffeology defines smoothness via plots— from of Euclidean spaces into the space itself, allowing for greater flexibility in handling singular or infinite-dimensional structures. This difference means that every differential space admits a diffeology, but not conversely, as diffeological spaces can incorporate pathological plots that do not arise from derivations, enabling diffeology to model spaces like certain more naturally without the algebraic constraints of . In relation to Frölicher spaces, diffeology shares the emphasis on sets equipped with families of smooth maps to and from , but diffeology prioritizes the plots (maps into the space) as the primary data for defining the structure, while Frölicher spaces balance both directions through a compatibility condition on the generated . This plot-centric approach in diffeology facilitates easier constructions of and , distinguishing it from Frölicher spaces, which may impose stricter conditions on the interchange of maps, though both frameworks generalize to or . Diffeological quotients offer a concrete way to model and , where the diffeology on the quotient captures the orbifold structure induced by , equivalent to Satake's V-manifolds or , by equipping the orbit space with plots that respect the . Furthermore, diffeology realizes ∞-Lie groupoids through diffeological groupoids, where the objects and arrows are diffeological spaces with , providing a smooth analogue to that extends beyond finite-dimensional Lie groupoids while preserving and orbit spaces.

References

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