nLab synthetic tangent bundle

Contents

Context

Synthetic differential geometry

synthetic differential geometry

Introductions

from point-set topology to differentiable manifolds

geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry

Differentials

V-manifolds

smooth space

Tangency

The magic algebraic facts

Theorems

Axiomatics

cohesion

infinitesimal cohesion

tangent cohesion

differential cohesion

graded differential cohesion

singular cohesion

id ⊣ id ∨ ∨ fermionic ⇉ ⊣ ⇝ bosonic ⊥ ⊥ bosonic ⇝ ⊣ Rh rheonomic ∨ ∨ reduced ℜ ⊣ ℑ infinitesimal ⊥ ⊥ infinitesimal ℑ ⊣ & étale ∨ ∨ cohesive ʃ ⊣ ♭ discrete ⊥ ⊥ discrete ♭ ⊣ ♯ continuous ∨ ∨ ∅ ⊣ * \array{ && id &\dashv& id \\ && \vee && \vee \\ &\stackrel{fermionic}{}& \rightrightarrows &\dashv& \rightsquigarrow & \stackrel{bosonic}{} \\ && \bot && \bot \\ &\stackrel{bosonic}{} & \rightsquigarrow &\dashv& \mathrm{R}\!\!\mathrm{h} & \stackrel{rheonomic}{} \\ && \vee && \vee \\ &\stackrel{reduced}{} & \Re &\dashv& \Im & \stackrel{infinitesimal}{} \\ && \bot && \bot \\ &\stackrel{infinitesimal}{}& \Im &\dashv& \& & \stackrel{\text{étale}}{} \\ && \vee && \vee \\ &\stackrel{cohesive}{}& \esh &\dashv& \flat & \stackrel{discrete}{} \\ && \bot && \bot \\ &\stackrel{discrete}{}& \flat &\dashv& \sharp & \stackrel{continuous}{} \\ && \vee && \vee \\ && \emptyset &\dashv& \ast }

Models

Lie theory, ∞-Lie theory

differential equations, variational calculus

Chern-Weil theory, ∞-Chern-Weil theory

Cartan geometry (super, higher)

Contents

Idea

In synthetic differential geometry, the tangent bundle of an object XX is the internal hom X 𝔻 1X^{\mathbb{D}^1} out of the 1d first order infinitesimal disk 𝔻 1\mathbb{D}^1, equipped with the projection to XX induced from the unique point *→𝔻 1\ast \to \mathbb{D}^1:

X (*→𝔻 1):X (𝔻 1)⟶X. X^{(\ast \to \mathbb{D}^1)} \;\colon\; X^{(\mathbb{D}^1)} \longrightarrow X \,.

(Here we are using that the internal hom-functor (−) (−)(-)^{(-)} is a contravariant functor in its “exponent” variable.)

This makes manifest and precise the intuitive idea that a tangent vector on XX is an “infinitesimal curve” in XX, see also the Examples below.

In this formulation the operation of differentiation is simply the internal hom-functor:

Given a function:

X⟶fY. X \overset{f}{\longrightarrow} Y \,.

its differential is its image under the internal hom (−) (𝔻 1)(-)^{(\mathbb{D}^1)}:

X (𝔻 1)⟶AAf (𝔻 1)AAY (𝔻 1). X^{(\mathbb{D}^1)} \overset{ \phantom{AA} f^{(\mathbb{D}^1)} \phantom{AA} }{\longrightarrow} Y^{(\mathbb{D}^1)} \,.

Examples

In a standard model for synthetic differential geometry/differential cohesion such as the Cahiers topos H\mathbf{H}, for X∈SmthMfd↪yHX \in SmthMfd \overset{y}{\hookrightarrow} \mathbf{H} an ordinary smooth manifold, its synthetic tangent bundle coincides with the traditional tangent bundle TX→pXT X \overset{p}{\to} X:

X (𝔻 1) ≃ TX X (*→𝔻 1)↓ ↓ p X X * ≃ X \array{ X^{(\mathbb{D}^1)} & \simeq & T X \\ {}^{\mathllap{ X^{ (\ast \to \mathbb{D}^1) } }}\big\downarrow && \big\downarrow{}^{ \mathrlap{p_X} } \\ X^{\ast} & \simeq & X }

Moreover, if Y∈SmthMfd↪HY \in SmthMfd \hookrightarrow \mathbf{H} is another smooth manifold, then a morphism

X⟶AAfAAY X \overset{\phantom{AA} f \phantom{AA} }{\longrightarrow} Y

is equivalently a smooth function in the traditional sense (i.e. the external Yoneda embedding-functor SmthMfd↪yHSmthMfd \overset{y}{\hookrightarrow} \mathbf{H} is fully faithful ) and its image under the internal hom is its traditional differentiation dfd f:

X (𝔻 1) ⟶AAf (𝔻 1)AA Y (𝔻 1) ≃↓ ↓ ≃ TX ⟶AAdfAA TY \array{ X^{(\mathbb{D}^1)} &\overset{ \phantom{AA} f^{(\mathbb{D}^1)} \phantom{AA} }{\longrightarrow}& Y^{(\mathbb{D}^1)} \\ {}^\simeq\big\downarrow && \big\downarrow{}^\simeq \\ T X &\overset{ \phantom{AA} d f \phantom{AA} }{\longrightarrow}& T Y }

This way the evident functoriality of the internal hom (−) (𝔻 1)(-)^{(\mathbb{D}^1)} is identified with the chain rule of traditional differentiation.

For more on this see

Properties

For Microlinear spaces

For XX a microlinear space the synthetic tangent bundle shares many of the expected properties of a tangent bundle.

References

For lecture notes see

Last revised on October 29, 2021 at 03:24:47. See the history of this page for a list of all contributions to it.