This post was translated from Korean by LLM (Kimi). The translation may contain errors or awkward sentences. The Korean original is the source of truth.

In this post we define tangent vectors on a manifold and the space they generate, the tangent space.

Motivation

In [Lee], a fairly lengthy portion of the beginning of Chapter 3 is devoted to justifying the definitions we will make; let us first briefly review this.

The simplest example of a manifold is \(\mathbb{R}^m\), and a slightly more complicated example is a surface contained in \(\mathbb{R}^m\). A tangent vector at a point \(p\) on this surface literally means vectors tangent to the surface at \(p\). If this surface is a two-dimensional surface in \(\mathbb{R}^3\), then collecting these vectors yields exactly the tangent plane at \(p\). However, generalizing this to a definition of tangent vectors on a manifold is not straightforward. In that definition, the existence of an ambient space \(\mathbb{R}^m\) containing the surface is essential, because we defined a manifold in a purely intrinsic way.

Instead, in the situation above we can observe that tangent vectors give rise to directional derivatives. That is, given any tangent vector \(v\), this vector assigns to each function \(f\) defined in a neighborhood of \(p\) the directional derivative in the \(v\)-direction

\[\lim_{t\rightarrow 0}\frac{f(p+tv)-f(p)}{t}\]

Our idea is to define this operator, the directional derivative, as the tangent vector.

Sheaf of Differentiable Functions

Let \(C^\infty(U)\) be the collection of \(C^\infty\) functions defined on an open set \(U\), and whenever \(V\subseteq U\) define the map \(\rho_{UV}:C^\infty(U)\rightarrow C^\infty(V)\) by

\[\rho_{UV}:f\mapsto f|_V\]

Then this structure becomes a sheaf of rings \(\mathcal{C}^\infty_M\) on \(M\). ([Topology] §Sheaves, ⁋Definition 1) The stalk of \(\mathcal{C}^\infty\) at any \(p\in M\) is written \(\mathcal{C}^\infty_{M,p}\), or simply \(\mathcal{C}^\infty_p\) when there is no danger of confusion. ([Topology] §Presheaves, ⁋Definition 9)

Proposition 1 For any manifold \(M\), \(\mathcal{C}^\infty_p\) has the structure of an \(\mathbb{R}\)-algebra.

Proof

To show this, it suffices to define operations on \(\mathcal{C}^\infty_p\). Choose two elements \(\mathbf{f},\mathbf{g}\) of \(\mathcal{C}^\infty_p\). Then there exist suitable open neighborhoods \(U,V\) of \(p\) such that we may regard \(\mathbf{f}\) and \(\mathbf{g}\) as the germs of \((f,U)\) and \((g,V)\), respectively. Now define \(\mathbf{f}+\mathbf{g}\) as the equivalence class of the function

\[(f|_{U\cap V}+g|_{U\cap V}, U\cap V)\]

In other words, to compute the sum of two germs \(\mathbf{f}\) and \(\mathbf{g}\), we find an open neighborhood of \(p\) on which both functions \(f,g\) are defined, and then compute the sum of \(f\) and \(g\) on this neighborhood. Of course, it is easy to see that this definition does not depend on the choice of representative.

Similarly, one can define multiplication of functions and scalar multiplication.

In fact, for scalar multiplication defined on \(\mathcal{C}^\infty_p\), since this can simply be thought of as multiplication by constant functions, we may regard \(\mathcal{C}^\infty_p\) as a ring rather than an algebra. Thus \((M,\mathcal{C}^\infty_M)\) becomes a ringed space. The next proposition shows that this space is a locally ringed space.

Proposition 2 The ring \(\mathcal{C}^\infty_p\) is a local ring, and its maximal ideal is given by

\[\mathfrak{m}_p=\{\mathbf{f}\in \mathcal{C}^\infty_p\mid \mathbf{f}(p)=0\}\]
Proof

First, the condition \(\mathbf{f}(p)=0\) is well defined. This is because all functions belonging to \(\mathbf{f}\) must have the same value at \(p\). It is not difficult to see that \(\mathfrak{m}_p\) is indeed an ideal.

Moreover, the maximality of \(\mathfrak{m}_p\) follows from the exactness of the diagram

\[0\longrightarrow \mathfrak{m}_p\longrightarrow \mathcal{C}^\infty_p\overset{\ev_p}{\longrightarrow}\mathbb{R}\longrightarrow 0\]

where the evaluation map \(\ev_p:\mathcal{C}^\infty_p\rightarrow\mathbb{R}\) is defined by \(\mathbf{f}\mapsto\mathbf{f}(p)\). This is because \(\mathcal{C}^\infty_p/\mathfrak{m}_p\) is the field \(\mathbb{R}\).

Tangent Vectors

Summarizing the preceding content without the language of sheaves is as follows.

We have decided to define a tangent vector at \(p\) as a directional derivative at the point $p$. This directional derivative is of course well defined for any function differentiable on all of \(M\), but differentiability is essentially a local property, so in fact the directional derivative of a function defined only on a suitable open neighborhood \(U\) of \(p\) can also be defined.1

Moreover, if two functions \(f,g\) agree on some open neighborhood \(U\) of \(p\), then their derivatives at \(p\) also coincide, so when dealing with directional derivatives they may be treated as identical. Thus the objects of our interest are no longer functions but equivalence classes of functions, which explicitly is as follows.

\[\mathcal{C}^\infty_p=\{(f,U)\mid f\in C^\infty(U)\}\big/{\sim},\qquad (f,U)\sim (g,V)\iff f\vert_W=g\vert_W\text{ for some $W\subseteq U\cap V$ open}\]

Let us write the equivalence class of \(f\) as \(\mathbf{f}\). Then the content of Proposition 1 is that scalar multiplication and addition, and even multiplication, are well defined on \(\mathcal{C}^\infty_p\), as in \(\mathbf{f}\mathbf{g},\mathbf{f}+\mathbf{g}\).

Now a tangent vector is a directional derivative that assigns a real number to each element of \(\mathcal{C}^\infty_p\). Here the derivative is defined as a linear map satisfying the Leibniz rule.

Definition 3 Let \(M\) be a manifold and \(p\in M\) a point. An \(\mathbb{R}\)-linear map \(v:\mathcal{C}^\infty_p\rightarrow\mathbb{R}\) satisfying the Leibniz rule

\[v(\mathbf{f}\mathbf{g})=\mathbf{f}(p)v(\mathbf{g})+\mathbf{g}(p)v(\mathbf{f})\]

is called a tangent vector of \(M\) at \(p\). The collection of tangent vectors of \(M\) at \(p\) is called the tangent space of \(M\) at \(p\), and is written \(T_pM\).

The next proposition states a fact that is already easy to guess.

Proposition 4 The \(T_pM\) defined in Definition 3 is an \(\mathbb{R}\)-vector space.

Proof

Since both \(\mathcal{C}^\infty_p\) and \(\mathbb{R}\) are \(\mathbb{R}\)-vector spaces, \(\Hom_\mathbb{R}(\mathcal{C}^\infty_p,\mathbb{R})\) is also an \(\mathbb{R}\)-vector space. Therefore, to show that the tangent space \(T_pM\) is indeed an \(\mathbb{R}\)-vector space as its name suggests, it suffices to show that \(T_pM\) is closed under addition and scalar multiplication. For example, since \(v+w\) is the linear map defined by

\[(v+w)(\mathbf{f})=v(\mathbf{f})+w(\mathbf{f})\]

to show that \(T_pM\) is closed under addition we compute

\[\begin{aligned}(v+w)(\mathbf{fg})&=v(\mathbf{fg})+w(\mathbf{fg})=\mathbf{f}(p)v(\mathbf{g})+\mathbf{g}(p)v(\mathbf{f})+\mathbf{f}(p)w(\mathbf{g})+\mathbf{g}(p)w(\mathbf{f})\\ &=\mathbf{f}(p)(v+w)(\mathbf{g})+\mathbf{g}(p)(v+w)(\mathbf{f})\end{aligned}\]

and confirm that \(v+w\) is also an element of \(T_pM\).

Moreover, for any tangent vector \(v\) and the constant function \(\mathbf{c}\) having the value \(c\) at every point, \(v(\mathbf{c})=0\) always holds. If we denote by \(\mathbf{1}\) the constant function with value \(1\), then since \(\mathbf{c}=c\cdot\mathbf{1}\) it suffices to show the following:

Lemma 6 For any tangent vector \(v\), we have \(v(\mathbf{1})=0\).

Proof \[v(\mathbf{1})=v(\mathbf{1}\cdot\mathbf{1})=\mathbf{1}(p)v(\mathbf{1})+\mathbf{1}(p)v(\mathbf{1})=v(\mathbf{1})+v(\mathbf{1})=2v(\mathbf{1}).\]

However, we still do not know what kind of space \(T_pM\) is. In particular, we do not yet know the dimension of \(T_pM\). We will examine this in the next post.


References

[War] Frank W. Warner. Foundations of Differentiable Manifolds and Lie Groups, Graduate texts in mathematics, Springer, 2013
[Lee] John M. Lee. Introduction to Smooth Manifolds, Graduate texts in mathematics, Springer, 2012


  1. Functions defined only on \(U\) can be extended to all of \(M\) via a partition of unity, so in the present situation we need not distinguish the two. 

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