Inmathematics,nuclear spaces aretopological vector spaces that can be viewed as a generalization of finite-dimensionalEuclidean spaces and share many of their desirable properties. Nuclear spaces are however quite different fromHilbert spaces, another generalization of finite-dimensional Euclidean spaces. They were introduced byAlexander Grothendieck.

The topology on nuclear spaces can be defined by a family ofseminorms whoseunit balls decrease rapidly in size. Vector spaces whose elements are "smooth" in some sense tend to be nuclear spaces; a typical example of a nuclear space is the set ofsmooth functions on acompact manifold. All finite-dimensional vector spaces are nuclear. There are noBanach spaces that are nuclear, except for the finite-dimensional ones. In practice a sort of converse to this is often true: if a "naturally occurring" topological vector space isnot a Banach space, then there is a good chance that it is nuclear.

Much of the theory of nuclear spaces was developed byAlexander Grothendieck while investigating theSchwartz kernel theorem and published in (Grothendieck 1955). We now describe this motivation.

For any open subsets${\displaystyle {\mathrm{\Omega }}_1\subseteq {\mathbb{R}}^m}$ and${\displaystyle {\mathrm{\Omega }}_2\subseteq {\mathbb{R}}^n,}$ the canonical map${\displaystyle {\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\times {\mathrm{\Omega }}_2\right)\to L_b\left(C_c^{\mathrm{\infty }}\left({\mathrm{\Omega }}_2\right);{\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\right)\right)}$ is an isomorphism of TVSs (where${\displaystyle L_b\left(C_c^{\mathrm{\infty }}\left({\mathrm{\Omega }}_2\right);{\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\right)\right)}$ has thetopology of uniform convergence on bounded subsets) and furthermore, both of these spaces are canonically TVS-isomorphic to${\displaystyle {\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\right)\hat{\otimes }{\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_2\right)}$ (where since${\displaystyle {\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\right)}$ is nuclear, this tensor product is simultaneously theinjective tensor product andprojective tensor product).^[1] In short, the Schwartz kernel theorem states that:$${\displaystyle {\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\times {\mathrm{\Omega }}_2\right)\cong {\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\right)\hat{\otimes }{\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_2\right)\cong L_b\left(C_c^{\mathrm{\infty }}\left({\mathrm{\Omega }}_2\right);{\mathcal{D}}^{\mathrm{\prime }}\left({\mathrm{\Omega }}_1\right)\right)}$$where all of theseTVS-isomorphisms are canonical.

This result is false if one replaces the space${\displaystyle C_c^{\mathrm{\infty }}}$ with${\displaystyle L^2}$ (which is areflexive space that is even isomorphic to its own strong dual space) and replaces${\displaystyle {\mathcal{D}}^{\mathrm{\prime }}}$ with the dual of this${\displaystyle L^2}$ space.^[2] Why does such a nice result hold for the space of distributions and test functions but not for theHilbert space${\displaystyle L^2}$ (which is generally considered one of the "nicest" TVSs)? This question led Grothendieck to discover nuclear spaces,nuclear maps, and theinjective tensor product.

Another set of motivating examples comes directly from geometry and smooth manifold theory^{[3]appendix 2}. Given smooth manifolds${\displaystyle M,N}$ and a locally convex Hausdorff topological vector space, then there are the following isomorphisms of nuclear spaces

• ${\displaystyle C^{\mathrm{\infty }}(M)\otimes C^{\mathrm{\infty }}(N)\cong C^{\mathrm{\infty }}(M\times N)}$
• ${\displaystyle C^{\mathrm{\infty }}(M)\otimes F\cong \{f:M\to F:f\text{ is smooth }\}}$

This section lists some of the more common definitions of a nuclear space. The definitions below are all equivalent. Note that some authors use a more restrictive definition of a nuclear space, by adding the condition that the space should also be aFréchet space. (This means that the space is complete and the topology is given by acountable family of seminorms.)

The following definition was used by Grothendieck to define nuclear spaces.^[4]

Definition 0: Let${\displaystyle X}$ be a locally convex topological vector space. Then${\displaystyle X}$ is nuclear if for every locally convex space${\displaystyle Y,}$ the canonical vector space embedding${\displaystyle X{\otimes }_{\pi }Y\to {\mathcal{B}}_{\epsilon }\left(X_{\sigma }^{\mathrm{\prime }},Y_{\sigma }^{\mathrm{\prime }}\right)}$ is an embedding of TVSs whose image is dense in the codomain (where the domain${\displaystyle X{\otimes }_{\pi }Y}$ is theprojective tensor product and the codomain is the space of all separately continuous bilinear forms on${\displaystyle X_{\sigma }^{\mathrm{\prime }}\times Y_{\sigma }^{\mathrm{\prime }}}$ endowed with thetopology of uniform convergence on equicontinuous subsets).

We start by recalling some background. Alocally convex topological vector space${\displaystyle X}$ has a topology that is defined by some family ofseminorms. For every seminorm, the unit ball is a closed convex symmetric neighborhood of the origin, and conversely every closed convex symmetric neighborhood of 0 is the unit ball of some seminorm. (For complex vector spaces, the condition "symmetric" should be replaced by "balanced".) If${\displaystyle p}$ is a seminorm on${\displaystyle X,}$ then${\displaystyle X_p}$ denotes theBanach space given bycompleting theauxiliary normed space using the seminorm${\displaystyle p.}$ There is a natural map${\displaystyle X\to X_p}$ (not necessarily injective).

If${\displaystyle q}$ is another seminorm, larger than${\displaystyle p}$ (pointwise as a function on${\displaystyle X}$), then there is a natural map from${\displaystyle X_q}$ to${\displaystyle X_p}$ such that the first map factors as${\displaystyle X\to X_q\to X_p.}$ These maps are always continuous. The space${\displaystyle X}$ is nuclear when a stronger condition holds, namely that these maps arenuclear operators. The condition of being a nuclear operator is subtle, and more details are available in the corresponding article.

Definition 1: Anuclear space is a locally convex topological vector space such that for every seminorm${\displaystyle p}$ we can find a larger seminorm${\displaystyle q}$ so that the natural map${\displaystyle X_q\to X_p}$ isnuclear.

Informally, this means that whenever we are given the unit ball of some seminorm, we can find a "much smaller" unit ball of another seminorm inside it, or that every neighborhood of 0 contains a "much smaller" neighborhood. It is not necessary to check this condition for all seminorms${\displaystyle p}$; it is sufficient to check it for a set of seminorms that generate the topology, in other words, a set of seminorms that are asubbase for the topology.

Instead of using arbitrary Banach spaces and nuclear operators, we can give a definition in terms ofHilbert spaces andtrace class operators, which are easier to understand. (On Hilbert spaces nuclear operators are often called trace class operators.)We will say that a seminorm${\displaystyle p}$ is aHilbert seminorm if${\displaystyle X_p}$ is a Hilbert space, or equivalently if${\displaystyle p}$ comes from a sesquilinear positive semidefinite form on${\displaystyle X.}$

Definition 2: Anuclear space is a topological vector space with a topology defined by a family of Hilbert seminorms, such that for every Hilbert seminorm${\displaystyle p}$ we can find a larger Hilbert seminorm${\displaystyle q}$ so that the natural map from${\displaystyle X_q}$ to${\displaystyle X_p}$ istrace class.

Some authors prefer to useHilbert–Schmidt operators rather than trace class operators. This makes little difference, because every trace class operator is Hilbert–Schmidt, and the product of two Hilbert–Schmidt operators is of trace class.

Definition 3: Anuclear space is a topological vector space with a topology defined by a family of Hilbert seminorms, such that for every Hilbert seminorm${\displaystyle p}$ we can find a larger Hilbert seminorm${\displaystyle q}$ so that the natural map from${\displaystyle X_q}$ to${\displaystyle X_p}$ is Hilbert–Schmidt.

If we are willing to use the concept of a nuclear operator from an arbitrary locally convex topological vector space to a Banach space, we can give shorter definitions as follows:

Definition 4: Anuclear space is a locally convex topological vector space such that for every seminorm${\displaystyle p}$ the natural map from${\displaystyle X\to X_p}$ isnuclear.

Definition 5: Anuclear space is a locally convex topological vector space such that every continuous linear map to a Banach space is nuclear.

Grothendieck used a definition similar to the following one:

Definition 6: Anuclear space is a locally convex topological vector space${\displaystyle A}$ such that for every locally convex topological vector space${\displaystyle B}$ the natural map from the projective to the injective tensor product of${\displaystyle A}$ and${\displaystyle B}$ is an isomorphism.

In fact it is sufficient to check this just for Banach spaces${\displaystyle B,}$ or even just for the single Banach space${\displaystyle {\ell }^1}$ of absolutely convergent series.

Let${\displaystyle X}$ be a Hausdorff locally convex space. Then the following are equivalent:

1. ${\displaystyle X}$ is nuclear;
2. for any locally convex space${\displaystyle Y,}$ the canonical vector space embedding${\displaystyle X{\otimes }_{\pi }Y\to {\mathcal{B}}_{ϵ}\left(X_{\sigma }^{\mathrm{\prime }},Y_{\sigma }^{\mathrm{\prime }}\right)}$ is an embedding of TVSs whose image is dense in the codomain;
3. for anyBanach space${\displaystyle Y,}$ the canonical vector space embedding${\displaystyle X{\hat{\otimes }}_{\pi }Y\to X{\hat{\otimes }}_{ϵ}Y}$ is a surjective isomorphism of TVSs;^[5]
4. for any locally convex Hausdorff space${\displaystyle Y,}$ the canonical vector space embedding${\displaystyle X{\hat{\otimes }}_{\pi }Y\to X{\hat{\otimes }}_{ϵ}Y}$ is a surjective isomorphism of TVSs;^[5]
5. the canonical embedding of${\displaystyle {\ell }^1[\mathbb{N},X]}$ in${\displaystyle {\ell }^1(\mathbb{N},X)}$ is a surjective isomorphism of TVSs;^[6]
6. the canonical map of${\displaystyle {\ell }^1{\hat{\otimes }}_{\pi }X\to {\ell }^1{\hat{\otimes }}_{ϵ}X}$ is a surjective TVS-isomorphism.^[6]
7. for any seminorm${\displaystyle p}$ we can find a larger seminorm${\displaystyle q}$ so that the natural map${\displaystyle X_q\to X_p}$ isnuclear;
8. for any seminorm${\displaystyle p}$ we can find a larger seminorm${\displaystyle q}$ so that the canonical injection${\displaystyle X_p^{\mathrm{\prime }}\to X_q^{\mathrm{\prime }}}$ is nuclear;^[5]
9. the topology of${\displaystyle X}$ is defined by a family of Hilbert seminorms, such that for any Hilbert seminorm${\displaystyle p}$ we can find a larger Hilbert seminorm${\displaystyle q}$ so that the natural map${\displaystyle X_q\to X_p}$ istrace class;
10. ${\displaystyle X}$ has a topology defined by a family of Hilbert seminorms, such that for any Hilbert seminorm${\displaystyle p}$ we can find a larger Hilbert seminorm${\displaystyle q}$ so that the natural map${\displaystyle X_q\to X_p}$ is Hilbert–Schmidt;
11. for any seminorm${\displaystyle p}$ the natural map from${\displaystyle X\to X_p}$ isnuclear.
12. any continuous linear map to a Banach space is nuclear;
13. every continuous seminorm on${\displaystyle X}$ is prenuclear;^[7]
14. everyequicontinuous subset of${\displaystyle X^{\mathrm{\prime }}}$ is prenuclear;^[7]
15. every linear map from a Banach space into${\displaystyle X^{\mathrm{\prime }}}$ that transforms the unit ball into an equicontinuous set, is nuclear;^[5]
16. the completion of${\displaystyle X}$ is a nuclear space;

If${\displaystyle X}$ is aFréchet space then the following are equivalent:

1. ${\displaystyle X}$ is nuclear;
2. every summable sequence in${\displaystyle X}$ is absolutely summable;^[6]
3. the strong dual of${\displaystyle X}$ is nuclear;

• A locally convex Hausdorff space is nuclear if and only if its completion is nuclear.
• Every subspace of a nuclear space is nuclear.^[8]
• Every Hausdorff quotient space of a nuclear space is nuclear.^[8]
• The inductive limit of a countable sequence of nuclear spaces is nuclear.^[8]
• The locally convex direct sum of a countable sequence of nuclear spaces is nuclear.^[8]
• The strong dual of a nuclear Fréchet space is nuclear.^[9]
  • In general, the strong dual of a nuclear space may fail to be nuclear.^[9]
• A Fréchet space whose strong dual is nuclear is itself nuclear.^[9]
• The limit of a family of nuclear spaces is nuclear.^[8]
• The product of a family of nuclear spaces is nuclear.^[8]
• The completion of a nuclear space is nuclear (and in fact a space is nuclear if and only if its completion is nuclear).
• Thetensor product of two nuclear spaces is nuclear.
• Theprojective tensor product, as well as its completion, of two nuclear spaces is nuclear.^[10]

Suppose that${\displaystyle X,Y,}$ and${\displaystyle N}$ are locally convex space with${\displaystyle N}$ is nuclear.

• If${\displaystyle N}$ is nuclear then the vector space of continuous linear maps${\displaystyle L_{\sigma }(X,N)}$ endowed with the topology of simple convergence is a nuclear space.^[9]
• If${\displaystyle X}$ is asemi-reflexive space whose strong dual is nuclear and if${\displaystyle N}$ is nuclear then the vector space of continuous linear maps${\displaystyle L_b(X,N)}$ (endowed with the topology of uniform convergence on bounded subsets of${\displaystyle X}$ ) is a nuclear space.^[11]

If${\displaystyle d}$ is a set of any cardinality, then${\displaystyle {\mathbb{R}}^d}$ and${\displaystyle {\mathbb{C}}^d}$ (with theproduct topology) are both nuclear spaces.^[12]

A relatively simple infinite-dimensional example of a nuclear space is the space of all rapidly decreasing sequences${\displaystyle c=\left(c_1,c_2,\dots \right).}$ ("Rapidly decreasing" means that${\displaystyle c_{n}p(n)}$ is bounded for any polynomial${\displaystyle p}$). For each real number${\displaystyle s,}$ it is possible to define a norm${\displaystyle \Vert \cdot {\Vert }_s}$ by$${\displaystyle \Vert c{\Vert }_s=\underset{}{sup}\left|c_n\right|n^s}$$If the completion in this norm is${\displaystyle C_s,}$ then there is a natural map from${\displaystyle C_s\to C_t}$ whenever${\displaystyle s\ge t,}$ and this is nuclear whenever${\displaystyle s>t+1}$ essentially because the series${\displaystyle \sum n^{t-s}}$ is then absolutely convergent. In particular for each norm${\displaystyle \Vert \cdot {\Vert }_t}$ this is possible to find another norm, say${\displaystyle \Vert \cdot {\Vert }_{t+1},}$ such that the map${\displaystyle C_{t+2}\to C_t}$ is nuclear. So the space is nuclear.

• The space of smooth functions on any compact manifold is nuclear.
• TheSchwartz space of smooth functions on${\displaystyle {\mathbb{R}}^n}$ for which the derivatives of all orders are rapidly decreasing is a nuclear space.
• The space of entire holomorphic functions on the complex plane is nuclear.
• Thespace of distributions${\displaystyle {\mathcal{D}}^{\mathrm{\prime }},}$ the strong dual of${\displaystyle \mathcal{D},}$ is nuclear.^[11]

Nuclear spaces are in many ways similar to finite-dimensional spaces and have many of their good properties.

• Every finite-dimensional Hausdorff space is nuclear.
• A Fréchet space is nuclear if and only if its strong dual is nuclear.
• Everybounded subset of a nuclear space is precompact (recall that a set is precompact if its closure in the completion of the space is compact).^[13] This is analogous to theHeine-Borel theorem. In contrast, no infinite-dimensional normed space has this property (although the finite-dimensional spaces do).
• If${\displaystyle X}$ is aquasi-complete (i.e. all closed and bounded subsets are complete) nuclear space then${\displaystyle X}$ has theHeine-Borel property.^[14]
• A nuclearquasi-completebarrelled space is aMontel space.
• Every closed equicontinuous subset of the dual of a nuclear space is a compact metrizable set (for the strong dual topology).
• Every nuclear space is a subspace of a product of Hilbert spaces.
• Every nuclear space admits a basis of seminorms consisting of Hilbert norms.
• Every nuclear space is a Schwartz space.
• Every nuclear space possesses the approximation property.^[15]
• Any subspace and any quotient space by a closed subspace of a nuclear space is nuclear.
• If${\displaystyle A}$ is nuclear and${\displaystyle B}$ is any locally convex topological vector space, then the natural map from the projective tensor product ofA and${\displaystyle B}$ to the injective tensor product is an isomorphism. Roughly speaking this means that there is only one sensible way to define the tensor product. This property characterizes nuclear spaces${\displaystyle A.}$
• In the theory of measures on topological vector spaces, a basic theorem states that any continuouscylinder set measure on the dual of a nuclear Fréchet space automatically extends to aRadon measure. This is useful because it is often easy to construct cylinder set measures on topological vector spaces, but these are not good enough for most applications unless they are Radon measures (for example, they are not even countably additive in general).

Much of the theory of nuclear spaces was developed byAlexander Grothendieck while investigating theSchwartz kernel theorem and published in (Grothendieck 1955). We have the following generalization of the theorem.

Schwartz kernel theorem:^[9] Suppose that${\displaystyle X}$ is nuclear,${\displaystyle Y}$ is locally convex, and${\displaystyle v}$ is a continuous bilinear form on${\displaystyle X\times Y.}$ Then${\displaystyle v}$ originates from a space of the form${\displaystyle X_{A^{\mathrm{\prime }}}^{\mathrm{\prime }}{\hat{\otimes }}_{ϵ}{Y}_{B^{\mathrm{\prime }}}^{\mathrm{\prime }}}$ where${\displaystyle A^{\mathrm{\prime }}}$ and${\displaystyle B^{\mathrm{\prime }}}$ are suitable equicontinuous subsets of${\displaystyle X^{\mathrm{\prime }}}$ and${\displaystyle Y^{\mathrm{\prime }}.}$ Equivalently,${\displaystyle v}$ is of the form,$${\displaystyle v(x,y)=\sum _{i=1}^{\mathrm{\infty }}{\lambda }_i⟨x,x_i^{\mathrm{\prime }}⟩⟨y,y_i^{\mathrm{\prime }}⟩\text{ for all }(x,y)\in X\times Y}$$where${\displaystyle \left({\lambda }_i\right)\in {\ell }^1}$ and each of${\displaystyle \left\{x_1^{\mathrm{\prime }},x_2^{\mathrm{\prime }},\dots \right\}}$ and${\displaystyle \left\{y_1^{\mathrm{\prime }},y_2^{\mathrm{\prime }},\dots \right\}}$ are equicontinuous. Furthermore, these sequences can be taken to be null sequences (that is, convergent to 0) in${\displaystyle X_{A^{\mathrm{\prime }}}^{\mathrm{\prime }}}$ and${\displaystyle Y_{B^{\mathrm{\prime }}}^{\mathrm{\prime }},}$ respectively.

Any continuouspositive-definite functional${\displaystyle C}$ on a nuclear space${\displaystyle A}$ is called acharacteristic functional if${\displaystyle C(0)=1,}$ and for any${\displaystyle z_j\in \mathbb{C},}$${\displaystyle x_j\in A}$ and${\displaystyle j,k=1,\dots ,n,}$^[16][17]$${\displaystyle \sum _{j=1}^n\sum _{k=1}^n{z}_j{\overline{z}}_{k}C(x_j-x_k)\ge 0.}$$

Given a characteristic functional on a nuclear space${\displaystyle A,}$ theBochner–Minlos theorem (afterSalomon Bochner andRobert Adol'fovich Minlos) guarantees the existence and uniqueness of a correspondingprobability measure${\displaystyle \mu }$ on the dual space${\displaystyle A^{\mathrm{\prime }}}$ such that$${\displaystyle C(y)={\int }_{A^{\mathrm{\prime }}}{e}^{i⟨x,y⟩}d\mu (x),}$$

where${\displaystyle C(y)}$ is theFourier-Stieltjes transform of${\displaystyle \mu }$, thereby extending theinverse Fourier transform to nuclear spaces.^[18]

In particular, if${\displaystyle A}$ is the nuclear space$${\displaystyle A=\bigcap _{k=0}^{\mathrm{\infty }}{H}_k,}$$where${\displaystyle H_k}$ are Hilbert spaces, the Bochner–Minlos theorem guarantees the existence of a probability measure with the characteristic function${\displaystyle e^{-\frac{1}{2}\Vert y{\Vert }_{H_0}^2},}$ that is, the existence of the Gaussian measure on thedual space. Such measure is calledwhite noise measure. When${\displaystyle A}$ is the Schwartz space, the correspondingrandom element is arandomdistribution.

Astrongly nuclear space is a locally convex topological vector space such that for any seminorm${\displaystyle p}$ there exists a larger seminorm${\displaystyle q}$ so that the natural map${\displaystyle X_q\to X_p}$ is a stronglynuclear.

• Auxiliary normed space
• Fredholm kernel – type of a kernel on a Banach space
• Injective tensor product
• Locally convex topological vector space – a vector space with a topology defined by convex open sets
• Nuclear operator
• Projective tensor product – a tensor product defined on two topological vector spaces
• Rigged Hilbert space – a construction linking the study of "bound" and continuous eigenvalues in functional analysis
• Trace class – the class of compact operators for which a finite trace can be defined
• Topological vector space – a vector space with a notion of nearness

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• Operator theory
• Topological vector spaces
• Topological tensor products

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