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代数拓扑中的微分形式

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代数拓扑中的微分形式 pleut (August 10, 2026) 参考:GTM82及Loring W Tu于台湾大学的课程(录像公开在台大官网) Chapter De Rham Cohomology 1 Tensors and Forms 1.1 Tensors definition [ 𝑘 -tensor] A

代数拓扑中的微分形式

pleut
(October 8, 2026)

参考:GTM82及Loring W Tu于台湾大学的课程(录像公开在台大官网)

1 De Rham Cohomology

1.1 Tensors and Forms

1.1.1 Tensors

Definition 1.0.1 (𝑘-tensor).

A 𝑘-tensor on a vector space 𝑉 is a 𝑘-linear function

𝑉×⋯×𝑉⏟__⏟__⏟𝑘 times⟶ℝ.
Example 1.0.1 ( Dual Space).

The dual space of a vector space 𝑉 is

𝑉∨={𝑓:𝑉→ℝ∣𝑓 is linear}.

Elements of 𝑉∨ are precisely 1-tensors on 𝑉.

Definition 1.0.2 (Alternating 𝑘-tensor).

A 𝑘-tensor 𝛼 is alternating if for any permutation 𝜎∈𝑆𝑘,

𝛼(𝑉𝜎(1),…,𝑉𝜎(𝑘))=sgn⁡(𝜎)𝛼(𝑉1,…,𝑉𝑘).

We denote by 𝐴𝑘(𝑉) the space of alternating 𝑘-tensors on 𝑉.

Remark 1.0.1.
  1. 1.

    Elements of 𝑉∨ are automatically alternating, i.e. 𝑉∨=𝐴1(𝑉)

  2. 2.

    The k-tensor and alternating k-tensor form two vector spaces, the vector space formed by alternating k-tensor is a subspace of k-tensor’s.

Example 1.0.2.

For 𝑉=ℝ3, the determinant det(𝑎,𝑏,𝑐) for 𝑎,𝑏,𝑐∈ℝ3 is a 3-linear alternating tensor.

Definition 1.0.3 (Wedge Product).

If 𝛼∈𝐴𝑘(𝑉) and 𝛽∈𝐴𝑙(𝑉), then 𝛼∧𝛽∈𝐴𝑘+𝑙(𝑉) is defined by

(𝛼∧𝛽)(𝑉1,…,𝑉𝑘+𝑙)=1𝑘!𝑙!∑𝜎∈𝑆𝑘+𝑙sgn⁡(𝜎)𝛼(𝑉𝜎(1),…,𝑉𝜎(𝑘))𝛽(𝑉𝜎(𝑘+1),…,𝑉𝜎(𝑘+𝑙)).
Example 1.0.3.

If 𝛼,𝛽∈𝐴1(𝑉), then

(𝛼∧𝛽)(𝑉1,𝑉2)=𝛼(𝑉1)𝛽(𝑉2)−𝛼(𝑉2)𝛽(𝑉1).
Proposition 1.0.1 (Basis of Alternating Tensors).

If {𝑎1,…,𝑎𝑛} is a basis for 𝑉∨, then

{𝑎𝑖1∧⋯∧𝑎𝑖𝑘∣1≤𝑖1<⋯<𝑖𝑘≤𝑛}

is a basis for 𝐴𝑘(𝑉).

Let 𝑈 be an open subset of ℝ𝑛, and let 𝑝∈𝑈. The tangent space at 𝑝 is

𝑇𝑝𝑈≅ℝ𝑛,

with basis {𝜕𝜕𝑥1∣𝑝,…,𝜕𝜕𝑥𝑛∣𝑝}.

1.1.2 Differential Forms

Definition 1.0.4 (Differential Form).

A 𝑘-form on 𝑈 is an assignment to each point 𝑝∈𝑈 of an alternating 𝑘-tensor

𝜔𝑝:𝑇𝑝𝑈×⋯×𝑇𝑝𝑈⏟___⏟___⏟𝑘 times⟶ℝ.

Equivalently, a 𝑘-form is a function

𝜔:𝑈⟶⋃𝑝∈𝑈𝐴𝑘(𝑇𝑝𝑈).
Remark 1.0.2.

k-form forms a vector space.

Definition 1.0.5 (Differential of a Function).

For 𝑓∈𝐶∞(𝑈), define the 1-form 𝑑𝑓 by

(𝑑𝑓)𝑝(𝑣)=𝑣𝑓=𝑛∑𝑖=1𝑣𝑖𝜕𝑓𝜕𝑥𝑖(𝑝),

where 𝑣=∑𝑣𝑖𝜕𝜕𝑥𝑖∣𝑝∈𝑇𝑝𝑈.

The 𝑥𝑖 can be viewed as a function, which gives the i-th coordinate.
Then for each 𝑖=1,…,𝑛, the 1-form 𝑑𝑥𝑖, by definition

(𝑑𝑥𝑖)𝑝(𝜕𝜕𝑥𝑗∣𝑝)=𝛿𝑖𝑗.
(𝑑𝑥𝑖)𝑝(𝑣)=𝑣𝑥𝑖=𝑛∑𝑗=1𝑣𝑗𝜕𝑓𝜕𝑥𝑗(𝑥𝑖)=𝑣𝑖

Thus 𝑑𝑥𝑖 picks out the 𝑖-th coordinate of a tangent vector.

Proposition 1.0.2 ( The expression of k-form in the local coordinate).

Every 𝑘-form 𝜔 on 𝑈 can be written uniquely as

𝜔=∑𝑖1<⋯<𝑖𝑘𝑎𝑖1⋯𝑖𝑘𝑑𝑥𝑖1∧⋯∧𝑑𝑥𝑖𝑘=:∑𝐼𝑎𝐼𝑑𝑥𝐼,

where 𝐼=(𝑖1,…,𝑖𝑘) with 1≤𝑖1<⋯<𝑖𝑘≤𝑛.

Definition 1.0.6 (Smooth Forms).

A 𝑘-form 𝜔=∑𝐼𝑎𝐼𝑑𝑥𝐼 is smooth (or 𝐶∞) if all coefficient functions 𝑎𝐼 are 𝐶∞. We denote

Ω𝑘(𝑈)={𝐶∞𝑘-forms on 𝑈}.
Theorem 1.1 (Exterior Derivative).

There exists a unique ℝ-linear map

𝑑:Ω𝑘(𝑈)⟶Ω𝑘+1(𝑈)

satisfying:

  1. 1.

    𝑑 is an antiderivation:

    𝑑(𝜔∧𝜏)=𝑑𝜔∧𝜏+(−1)𝑘𝜔∧𝑑𝜏,𝜔∈Ω𝑘(𝑈).

  2. 2.

    𝑑∘𝑑=0, i.e. 𝑑2=0.

  3. 3.

    On Ω0(𝑈)=𝐶∞(𝑈), 𝑑 is the usual differential: 𝑑𝑓=∑𝑖𝜕𝑓𝜕𝑥𝑖𝑑𝑥𝑖.

Remark 1.1.1.

For a 𝑘-form 𝜔=∑𝐼𝑎𝐼𝑑𝑥𝐼, the exterior derivative is given by

𝑑𝜔=∑𝐼𝑑𝑎𝐼∧𝑑𝑥𝐼=∑𝐼𝑛∑𝑗=1𝜕𝑎𝐼𝜕𝑥𝑗𝑑𝑥𝑗∧𝑑𝑥𝐼.

Let 𝑈⊆ℝ𝑛 be open. The sequence

0⟶Ω0(𝑈)𝑑0⟶Ω1(𝑈)𝑑1⟶⋯𝑑𝑛−1←←←←←←←→Ω𝑛(𝑈)⟶0

is called the de Rham complex of 𝑈. Since 𝑑𝑘∘𝑑𝑘−1=0, we have

Im⁡𝑑𝑘−1⊆ker⁡𝑑𝑘.
Definition 1.1.1 (Closed and Exact Forms).
  • •

    A 𝑘-form 𝜔∈Ω𝑘(𝑈) is closed if 𝑑𝜔=0. The space of closed 𝑘-forms is denoted

    𝑍𝑘(𝑈)=ker⁡𝑑𝑘.
  • •

    A 𝑘-form 𝜔∈Ω𝑘(𝑈) is exact if 𝜔=𝑑𝜂 for some 𝜂∈Ω𝑘−1(𝑈). The space of exact 𝑘-forms is denoted

    𝐵𝑘(𝑈)=Im⁡𝑑𝑘−1.

1.2 The De Rham Cohomology

1.2.1 De Rham Cohomology

Definition 1.1.2 (De Rham Cohomology).

The 𝑘-th de Rham cohomology of 𝑈 is the quotient vector space

𝐻𝑘(𝑈)=ker⁡𝑑𝑘Im⁡𝑑𝑘−1=𝑍𝑘(𝑈)𝐵𝑘(𝑈).
Example 1.1.1 ( Computation of 𝐻∗(ℝ)).

Consider the de Rham complex for 𝑈=ℝ:

0⟶Ω0(ℝ)𝑑0⟶Ω1(ℝ)⟶0.

Computation of 𝐻0(ℝ)

𝑍0(ℝ)={𝑓∈𝐶∞(ℝ)∣𝑑𝑓=0}.

Since 𝑑𝑓=𝑓′(𝑥)𝑑𝑥, we have 𝑑𝑓=0⟺𝑓′(𝑥)=0⟺𝑓 is constant. Thus

𝑍0(ℝ)≅ℝ.

Also,

𝐵0(ℝ)=Im⁡𝑑−1=0.

Therefore,

𝐻0(ℝ)=𝑍0(ℝ)/𝐵0(ℝ)≅ℝ.

Computation of 𝐻1(ℝ)

𝑍1(ℝ)={𝑔(𝑥)𝑑𝑥∣𝑑(𝑔(𝑥)𝑑𝑥)=0}.

But 𝑑(𝑔(𝑥)𝑑𝑥)=0 automatically, so

𝑍1(ℝ)={𝑔(𝑥)𝑑𝑥∣𝑔∈𝐶∞(ℝ)}≅𝐶∞(ℝ).

Next,

𝐵1(ℝ)={𝑑𝑓∣𝑓∈𝐶∞(ℝ)}={𝑓′(𝑥)𝑑𝑥∣𝑓∈𝐶∞(ℝ)}.

Given any 𝑔∈𝐶∞(ℝ), define

𝑓(𝑥)=∫𝑥0𝑔(𝑡)𝑑𝑡.

Then 𝑓∈𝐶∞(ℝ) and 𝑓′(𝑥)=𝑔(𝑥). Hence 𝑔(𝑥)𝑑𝑥=𝑑𝑓, so

𝑍1(ℝ)=𝐵1(ℝ).

Therefore,

𝐻1(ℝ)=0.
Proposition 1.1.1.

The de Rham cohomology of ℝ is

𝐻𝑘(ℝ)={ℝ,𝑘=0,0,𝑘≥1.

1.2.2 Cohomology with Compact Support

Definition 1.1.3 (Support of a Differential Form).

Let 𝑈⊆ℝ𝑛 be open, and let 𝜔∈Ω𝑘(𝑈) be a 𝑘-form. The zero set of 𝜔 is defined as

𝑍(𝜔)={𝑝∈𝑈∣𝜔𝑝=0}.

The support of 𝜔 is the closure in 𝑈 of the complement of the zero set:

supp⁡𝜔=cl𝑈⁡(𝑈∖𝑍(𝜔))=cl𝑈⁡(𝑍(𝜔)𝑐).

In other words, the support of 𝜔 is the smallest closed set outside which 𝜔 is identically zero.

Definition 1.1.4 (Compact Support Forms).

Let 𝑈⊆ℝ𝑛 be open. We denote by

Ω𝑘𝑐(𝑈)={𝜔∈Ω𝑘(𝑈)∣supp⁡𝜔 is compact in 𝑈}

the space of smooth 𝑘-forms with compact support.

Proposition 1.1.2 (Support is Decreasing under 𝑑).

For any 𝜔∈Ω𝑘𝑐(𝑈), we have

supp⁡(𝑑𝜔)⊆supp⁡𝜔.

In particular, if 𝜔 has compact support, then so does 𝑑𝜔.

Proof.

We prove the equivalent statement

(supp⁡𝜔)𝑐⊆(supp⁡𝑑𝜔)𝑐.

Let 𝑝∈(supp⁡𝜔)𝑐. Since supp⁡𝜔 is closed, there exists an open neighbourhood 𝑉⊆𝑈 of 𝑝 such that

𝑉⊆𝑈∖supp⁡𝜔.

Hence 𝜔≡0 on 𝑉. Therefore, 𝑑𝜔≡0 on 𝑉, which means

𝑝∉supp⁡(𝑑𝜔).

Thus 𝑝∈(supp⁡𝑑𝜔)𝑐, proving the inclusion. Consequently,

supp⁡(𝑑𝜔)⊆supp⁡𝜔.

Since supp⁡𝜔 is compact and supp⁡(𝑑𝜔) is closed, it follows that supp⁡(𝑑𝜔) is also compact. Hence 𝑑𝜔∈Ω𝑘+1𝑐(𝑈). ∎

Corollary 1.1.1.

The exterior derivative restricts to a linear map

𝑑:Ω𝑘𝑐(𝑈)⟶Ω𝑘+1𝑐(𝑈).

Thus the sequence

0⟶Ω0𝑐(𝑈)𝑑→Ω1𝑐(𝑈)𝑑→⋯𝑑→Ω𝑛𝑐(𝑈)⟶0

is a cochain complex, called the de Rham complex with compact support.

Definition 1.1.5 (Compact Support Cohomology).

The 𝑘-th de Rham cohomology with compact support of 𝑈 is the quotient

𝐻𝑘𝑐(𝑈)=𝑍𝑘𝑐(𝑈)𝐵𝑘𝑐(𝑈),

where

𝑍𝑘𝑐(𝑈)=ker⁡(𝑑:Ω𝑘𝑐(𝑈)→Ω𝑘+1𝑐(𝑈))

is the space of closed compactly supported 𝑘-forms, and

𝐵𝑘𝑐(𝑈)=Im⁡(𝑑:Ω𝑘−1𝑐(𝑈)→Ω𝑘𝑐(𝑈))

is the space of exact compactly supported 𝑘-forms.

Example 1.1.2 (𝐻∗𝑐(ℝ)).

Let us compute the compact support cohomology of ℝ. The complex is

0⟶Ω0𝑐(ℝ)𝑑→Ω1𝑐(ℝ)⟶0.

Computation of 𝐻0𝑐(ℝ): We have

𝑍0𝑐(ℝ)={𝑓∈𝐶∞𝑐(ℝ)∣𝑑𝑓=0}.

Since 𝑑𝑓=𝑓′(𝑥)𝑑𝑥, the condition 𝑑𝑓=0 implies 𝑓′(𝑥)=0, so 𝑓 is constant. But a compactly supported constant function on ℝ must be zero. Hence

𝑍0𝑐(ℝ)=0.

Therefore,

𝐻0𝑐(ℝ)=0.

Computation of 𝐻1𝑐(ℝ): First,

𝑍1𝑐(ℝ)={𝑔(𝑥)𝑑𝑥∣𝑔∈𝐶∞𝑐(ℝ)},

since every 1-form on ℝ is automatically closed. Also,

𝐵1𝑐(ℝ)={𝑑𝑓∣𝑓∈𝐶∞𝑐(ℝ)}={𝑓′(𝑥)𝑑𝑥∣𝑓∈𝐶∞𝑐(ℝ)}.

We claim that a compactly supported function 𝑔∈𝐶∞𝑐(ℝ) lies in 𝐵1𝑐(ℝ) if and only if

∫+∞−∞𝑔(𝑥)𝑑𝑥=0.

Indeed, if 𝑔=𝑓′ for some 𝑓∈𝐶∞𝑐(ℝ), then by the fundamental theorem of calculus,

∫+∞−∞𝑔(𝑥)𝑑𝑥=∫+∞−∞𝑓′(𝑥)𝑑𝑥=𝑓(+∞)−𝑓(−∞)=0.

Conversely, suppose 𝑔∈𝐶∞𝑐(ℝ) satisfies ∫+∞−∞𝑔(𝑥)𝑑𝑥=0. Define

𝑓(𝑥)=∫𝑥−∞𝑔(𝑡)𝑑𝑡.

Then 𝑓′(𝑥)=𝑔(𝑥). Moreover, for 𝑥 sufficiently large (outside the support of 𝑔), we have 𝑓(𝑥)=∫+∞−∞𝑔(𝑡)𝑑𝑡=0, so 𝑓 has compact support. Hence 𝑔∈𝐵1𝑐(ℝ).

Thus we have an exact sequence

0⟶𝐵1𝑐(ℝ)⟶𝑍1𝑐(ℝ)∫+∞−∞←←←←←←←←←→ℝ⟶0,

where the map is integration of the coefficient function. Therefore,

𝐻1𝑐(ℝ)=𝑍1𝑐(ℝ)𝐵1𝑐(ℝ)≅ℝ.

In summary,

𝐻𝑘𝑐(ℝ)={0,𝑘=0,ℝ,𝑘=1.
Remark 1.1.2.

Compare this with the ordinary de Rham cohomology of ℝ:

𝐻𝑘(ℝ)={ℝ,𝑘=0,0,𝑘≥1.

The two cohomology theories differ significantly: compact support cohomology “detects” the non-compactness of ℝ in degree 1, whereas ordinary cohomology detects it in degree 0.

1.3 Diffeomorphism Invariance

1.3.1 Pullback

Definition 1.1.6 (Pullback).

Let 𝐹:𝑀→𝑁 be a smooth map between smooth manifolds. The pullback

𝐹∗:Ω𝑘(𝑁)⟶Ω𝑘(𝑀)

is the unique linear map satisfying:

  1. 1.

    For 𝑔∈Ω0(𝑁)=𝐶∞(𝑁),

    𝐹∗𝑔=𝑔∘𝐹.
  2. 2.

    𝐹∗ commutes with addition, subtraction, wedge product, and the exterior derivative:

    𝐹∗(𝜔+𝜏)=𝐹∗𝜔+𝐹∗𝜏,𝐹∗(𝜔∧𝜏)=𝐹∗𝜔∧𝐹∗𝜏,𝐹∗(𝑑𝜔)=𝑑(𝐹∗𝜔).
  3. 3.

    For smooth maps 𝐹:𝑀→𝑁 and 𝐺:𝑁→𝑃,

    (𝐹∘𝐺)∗=𝐺∗∘𝐹∗.

In local coordinates: if 𝜔∈Ω𝑘(𝑁) is expressed on a chart (𝑉,𝑦1,…,𝑦𝑛) as

𝜔=∑𝑖1<⋯<𝑖𝑘𝑎𝑖1⋯𝑖𝑘𝑑𝑦𝑖1∧⋯∧𝑑𝑦𝑖𝑘,

then

𝐹∗𝜔=∑(𝑎𝑖1⋯𝑖𝑘∘𝐹)𝑑(𝑦𝑖1∘𝐹)∧⋯∧𝑑(𝑦𝑖𝑘∘𝐹).

Equivalently, if we write 𝐹𝑖=𝑦𝑖∘𝐹, then

𝐹∗𝜔=∑(𝑎𝑖1⋯𝑖𝑘∘𝐹)𝑑𝐹𝑖1∧⋯∧𝑑𝐹𝑖𝑘.
Proposition 1.1.3.

The pullback 𝐹∗:Ω𝑘(𝑁)→Ω𝑘(𝑀) induces a well-defined linear map on cohomology

𝐹∗:𝐻𝑘(𝑁)⟶𝐻𝑘(𝑀).

Proof.

We show that 𝐹∗ sends closed forms to closed forms and exact forms to exact forms.

If 𝜔 is closed, then 𝑑𝜔=0, so

𝑑(𝐹∗𝜔)=𝐹∗(𝑑𝜔)=𝐹∗(0)=0.

Thus 𝐹∗𝜔 is closed.

If 𝜔=𝑑𝜏 is exact, then

𝐹∗𝜔=𝐹∗(𝑑𝜏)=𝑑(𝐹∗𝜏),

which is exact. Hence 𝐹∗ maps the subspace of exact forms into exact forms.

Therefore, 𝐹∗ descends to a well-defined map on the quotient:

𝐹∗:𝐻𝑘(𝑁)⟶𝐻𝑘(𝑀),[𝜔]⟼[𝐹∗𝜔].

∎

Theorem 1.2 (Diffeomorphism Invariance).

If 𝐹:𝑀→𝑁 is a diffeomorphism, then the induced map

𝐹∗:𝐻𝑘(𝑁)⟶𝐻𝑘(𝑀)

is an isomorphism for every 𝑘.

Proof.

Let 𝐺:𝑁→𝑀 be the inverse diffeomorphism of 𝐹. Then 𝐹∘𝐺=id𝑁 and 𝐺∘𝐹=id𝑀. By the functoriality of pullback,

(𝐹∘𝐺)∗=𝐺∗∘𝐹∗=id𝐻∗(𝑁),

and

(𝐺∘𝐹)∗=𝐹∗∘𝐺∗=id𝐻∗(𝑀)⁡.

Thus 𝐹∗ has a two-sided inverse 𝐺∗, so 𝐹∗ is an isomorphism. ∎

Example 1.2.1 ( Intervals).

The tangent map

tan:(−𝜋2,𝜋2)⟶ℝ

is a diffeomorphism. Therefore,

tan∗:𝐻∗(ℝ)⟶𝐻∗(−𝜋2,𝜋2)

is an isomorphism. Hence

𝐻∗(−𝜋2,𝜋2)≅𝐻∗(ℝ).

Since any open interval (𝑎,𝑏) is diffeomorphic to (−𝜋2,𝜋2), we have

𝐻𝑘(𝑎,𝑏)≅{ℝ,𝑘=0,0,𝑘>0.
Remark 1.2.1.

If 𝐹:𝑁→𝑀 is a smooth map, then the pullback of a compactly supported form need not have compact support. However, for diffeomorphisms, the induced map on compact support cohomology also exists and is an isomorphism:

𝐹∗:𝐻𝑘𝑐(𝑀)⟶𝐻𝑘𝑐(𝑁).

Thus 𝐻∗𝑐(𝑀) is also a diffeomorphism invariant.

1.3.2 Exact Sequences and Cochain Complexes

Definition 1.2.1 (Exact Sequence).

A sequence of vector spaces and linear maps

⋯⟶𝑉𝑘−1𝑓𝑘−1←←←←←←←→𝑉𝑘𝑓𝑘⟶𝑉𝑘+1⟶⋯

is exact at 𝑉𝑘 if

ker⁡𝑓𝑘=Im⁡𝑓𝑘−1.

The sequence is exact if it is exact at every 𝑉𝑘 for all 𝑘∈ℤ.

Definition 1.2.2 (Short Exact Sequence).

A short exact sequence is an exact sequence of the form

0⟶𝐴𝑖→𝐵𝑗→𝐶⟶0.
Remark 1.2.2.

In a short exact sequence 0→𝐴𝑖→𝐵𝑗→𝐶→0:

  • •

    Exactness at 𝐴 means 𝑖 is injective.

  • •

    Exactness at 𝐶 means 𝑗 is surjective.

  • •

    Exactness at 𝐵 means ker⁡𝑗=Im⁡𝑖.

  • •

    Consequently, 𝐵/𝐴≅𝐶.

Definition 1.2.3 (Cochain Complex).

A cochain complex 𝐶∙ is a sequence of vector spaces and linear maps

⋯⟶𝐶𝑘−1𝑑𝑘−1←←←←←←←→𝐶𝑘𝑑𝑘⟶𝐶𝑘+1⟶⋯

such that

𝑑𝑘∘𝑑𝑘−1=0

for all 𝑘∈ℤ. The maps 𝑑𝑘 are called differentials or coboundary operators.

For a cochain complex 𝐶∙, its cohomology is defined as

𝐻𝑘(𝐶∙)=ker⁡𝑑𝑘Im⁡𝑑𝑘−1.
Definition 1.2.4 (Cochain Map).

A cochain map 𝜑:𝐴∙→𝐵∙ is a collection of linear maps

𝜑𝑘:𝐴𝑘⟶𝐵𝑘

such that for every 𝑘,

𝜑𝑘+1∘𝑑𝑘𝐴=𝑑𝑘𝐵∘𝜑𝑘.

That is, the following diagram commutes:

tikzcd diagram
Proposition 1.2.1.

A cochain map 𝜑:𝐴∙→𝐵∙ induces a linear map on cohomology

𝜑∗:𝐻𝑘(𝐴∙)⟶𝐻𝑘(𝐵∙).

Definition 1.2.5 (Short Exact Sequence of Cochain Complexes).

A sequence of cochain complexes

0⟶𝐴∙𝑖→𝐵∙𝑗→𝐶∙⟶0

is a short exact sequence of cochain complexes if for every 𝑘,

0⟶𝐴𝑘𝑖𝑘⟶𝐵𝑘𝑗𝑘⟶𝐶𝑘⟶0

is a short exact sequence of vector spaces, and 𝑖,𝑗 are cochain maps.

1.4 Mayer–Vietoris Sequence

1.4.1 The Zig–Zag Lemma

Theorem 1.3 (Zig–Zag Lemma).

Let

0⟶𝐴∙𝑖→𝐵∙𝑗→𝐶∙⟶0

be a short exact sequence of cochain complexes. Then there is a long exact sequence in cohomology:

tikzcd diagram

The maps 𝛿𝑘:𝐻𝑘(𝐶∙)→𝐻𝑘+1(𝐴∙) are called the connecting homomorphisms. We now describe their construction.

Construction of the Connecting Homomorphism.

Let [𝑐]∈𝐻𝑘(𝐶∙) be a cohomology class represented by 𝑐∈𝐶𝑘 with 𝑑𝐶𝑐=0.

  1. 1.

    Since 𝑗𝑘:𝐵𝑘→𝐶𝑘 is surjective, there exists 𝑏∈𝐵𝑘 such that

    𝑗𝑘(𝑏)=𝑐.
  2. 2.

    Since 𝑗 is a cochain map,

    𝑗𝑘+1(𝑑𝐵𝑏)=𝑑𝐶(𝑗𝑘𝑏)=𝑑𝐶𝑐=0.

    By exactness of the rows, there exists a unique 𝑎∈𝐴𝑘+1 such that

    𝑖𝑘+1(𝑎)=𝑑𝐵𝑏.

    Uniqueness follows from the injectivity of 𝑖𝑘+1.

  3. 3.

    We show that 𝑎 is closed:

    𝑖𝑘+2(𝑑𝐴𝑎)=𝑑𝐵(𝑖𝑘+1(𝑎))=𝑑𝐵(𝑑𝐵𝑏)=0.

    Since 𝑖𝑘+2 is injective, we have 𝑑𝐴𝑎=0. Thus 𝑎 defines a cohomology class [𝑎]∈𝐻𝑘+1(𝐴∙).

We define

𝛿𝑘[𝑐]=[𝑎]∈𝐻𝑘+1(𝐴∙).
Proposition 1.3.1.

The connecting homomorphism 𝛿𝑘 is well-defined, i.e. independent of the choices of 𝑏 and the representative 𝑐.

∎

Proof.

See standard references (e.g., Manifolds §25). The proof is a straightforward diagram chase. ∎

1.4.2 Partitions of Unity

To construct the Mayer–Vietoris sequence for de Rham cohomology, we need a technical tool: partitions of unity.

Definition 1.3.1 (Partition of Unity).

Let 𝑀 be a smooth manifold, and let {𝑈𝛼}𝛼∈𝐴 be an open cover of 𝑀. A 𝐶∞ partition of unity subordinate to {𝑈𝛼} is a collection of smooth functions

{𝜌𝛼:𝑀→ℝ}𝛼∈𝐴

satisfying:

  1. 1.

    0≤𝜌𝛼(𝑝)≤1 for all 𝑝∈𝑀 and all 𝛼∈𝐴.

  2. 2.

    supp⁡𝜌𝛼⊆𝑈𝛼 for each 𝛼∈𝐴.

  3. 3.

    The collection {supp⁡𝜌𝛼}𝛼∈𝐴 is locally finite: every point 𝑝∈𝑀 has a neighbourhood that intersects only finitely many supports.

  4. 4.

    For every 𝑝∈𝑀,

    ∑𝛼∈𝐴𝜌𝛼(𝑝)=1.

    (This sum is finite because of local finiteness.)

Theorem 1.4 (Existence of Partitions of Unity).

Every open cover of a smooth manifold admits a 𝐶∞ partition of unity subordinate to it.

Proof.

See standard references on smooth manifolds (e.g., Manifolds, Appendix C). ∎

1.4.3 The Mayer–Vietoris Theorem

Let 𝑀 be a smooth manifold, and let {𝑈,𝑉} be an open cover of 𝑀. We will construct a short exact sequence of cochain complexes that induces the Mayer–Vietoris long exact sequence in cohomology.

Define the following maps:

  • •

    The inclusion map

    𝑖:Ω𝑘(𝑀)⟶Ω𝑘(𝑈)⊕Ω𝑘(𝑉)

    given by

    𝑖(𝜔)=(𝜔|𝑈,𝜔|𝑉).
  • •

    The difference map

    𝑗:Ω𝑘(𝑈)⊕Ω𝑘(𝑉)⟶Ω𝑘(𝑈∩𝑉)

    given by

    𝑗(𝜔,𝜏)=𝜔|𝑈∩𝑉−𝜏|𝑈∩𝑉.
Proposition 1.4.1.

The sequence of cochain complexes

0⟶Ω∙(𝑀)𝑖→Ω∙(𝑈)⊕Ω∙(𝑉)𝑗→Ω∙(𝑈∩𝑉)⟶0

is short exact.

Proof.

We verify exactness at each stage.

Exactness at Ω𝑘(𝑀): The map 𝑖 is injective because if 𝜔|𝑈=0 and 𝜔|𝑉=0, then 𝜔=0 on 𝑀=𝑈∪𝑉.

Exactness at Ω𝑘(𝑈)⊕Ω𝑘(𝑉): Clearly Im⁡𝑖⊆ker⁡𝑗, since

𝑗(𝑖(𝜔))=𝑗(𝜔|𝑈,𝜔|𝑉)=𝜔|𝑈∩𝑉−𝜔|𝑈∩𝑉=0.

Conversely, suppose (𝜔,𝜏)∈ker⁡𝑗, so 𝜔|𝑈∩𝑉=𝜏|𝑈∩𝑉. We need to find 𝜂∈Ω𝑘(𝑀) such that 𝜂|𝑈=𝜔 and 𝜂|𝑉=𝜏. This is a gluing problem. Let {𝜌𝑈,𝜌𝑉} be a partition of unity subordinate to the cover {𝑈,𝑉}. Define

𝜂=𝜌𝑈𝜔+𝜌𝑉𝜏,

where 𝜌𝑈𝜔 is extended by zero outside 𝑈, and similarly for 𝜌𝑉𝜏. On 𝑈∩𝑉, 𝜔=𝜏, so

𝜂|𝑈∩𝑉=𝜌𝑈𝜔+𝜌𝑉𝜔=𝜔.

On 𝑈, the term 𝜌𝑉𝜏 is supported in 𝑉∩𝑈, and on 𝑉, 𝜌𝑈𝜔 is supported in 𝑈∩𝑉. Thus 𝜂 glues properly, and 𝑖(𝜂)=(𝜔,𝜏).

Exactness at Ω𝑘(𝑈∩𝑉): The map 𝑗 is surjective. For any 𝜔∈Ω𝑘(𝑈∩𝑉), we can extend it to a form on 𝑈 (using a bump function) and take (𝜔,0)∈Ω𝑘(𝑈)⊕Ω𝑘(𝑉), which satisfies 𝑗(𝜔,0)=𝜔. (Alternatively, use a partition of unity to construct the extension.) ∎

Theorem 1.5 (Mayer–Vietoris Sequence).

Let {𝑈,𝑉} be an open cover of a smooth manifold 𝑀. Then there is a long exact sequence in de Rham cohomology:

tikzcd diagram

Proof.

Apply the Zig–Zag lemma to the short exact sequence of cochain complexes

0⟶Ω∙(𝑀)𝑖→Ω∙(𝑈)⊕Ω∙(𝑉)𝑗→Ω∙(𝑈∩𝑉)⟶0.

∎

1.4.4 Applications

Example 1.5.1 (Cohomology of Disjoint Unions).

If 𝑀=𝐴⨿𝐵 is a disjoint union of smooth manifolds, then

𝐻𝑘(𝑀)≅𝐻𝑘(𝐴)⊕𝐻𝑘(𝐵).

This follows directly from the definition of differential forms on a disjoint union.

Example 1.5.2 (Cohomology in Degree 0).

If 𝑀 has 𝑚 connected components, then

𝐻0(𝑀)≅ℝ𝑚.

This is because a closed 0-form is a locally constant function, hence constant on each connected component.

Example 1.5.3 (Cohomology of 𝑆1).

Using the Mayer–Vietoris sequence, we can compute the cohomology of the circle 𝑆1. Let 𝑆1=𝑈∪𝑉, where 𝑈 and 𝑉 are two open arcs that cover the circle, and 𝑈∩𝑉 is a disjoint union of two intervals. Since intervals are contractible, 𝐻𝑘(𝑈)=𝐻𝑘(𝑉)=𝐻𝑘(𝑈∩𝑉)=0 for 𝑘≥1, and 𝐻0 of each is ℝ. The Mayer–Vietoris sequence gives

0⟶𝐻0(𝑆1)⟶ℝ⊕ℝ⟶ℝ⊕ℝ⟶𝐻1(𝑆1)⟶0.

A short computation yields

𝐻0(𝑆1)≅ℝ,𝐻1(𝑆1)≅ℝ,𝐻𝑘(𝑆1)=0(𝑘≥2).
Remark 1.5.1.

The Mayer–Vietoris sequence is an indispensable tool in algebraic topology. It can be used inductively to compute the cohomology of many manifolds by decomposing them into simpler pieces.

1.5 Homotopy Invariance

1.5.1 Homotopy

Definition 1.5.1 (Smooth Homotopy).

Let 𝑀 and 𝑁 be smooth manifolds. Two smooth maps

𝑓0,𝑓1:𝑀⟶𝑁

are smoothly homotopic if there exists a smooth map

𝐹:𝑀×[0,1]⟶𝑁

such that

𝐹(𝑥,0)=𝑓0(𝑥),𝐹(𝑥,1)=𝑓1(𝑥)for all 𝑥∈𝑀.

The map 𝐹 is called a smooth homotopy between 𝑓0 and 𝑓1. Here “smooth on 𝑀×[0,1]” means that 𝐹 can be extended to a smooth map on a neighbourhood of 𝑀×[0,1] in 𝑀×ℝ.

Definition 1.5.2 (Homotopy Equivalence).

A smooth map 𝑓:𝑀→𝑁 is a homotopy equivalence if there exists a smooth map 𝑔:𝑁→𝑀 such that

𝑔∘𝑓∼id𝑀,𝑓∘𝑔∼id𝑁⁡.

The map 𝑔 is called a homotopy inverse of 𝑓. In this case, 𝑀 and 𝑁 are said to have the same homotopy type. A manifold with the homotopy type of a point is called contractible.

Example 1.5.4 (Retraction of ℝ2∖{0} onto 𝑆1).

Consider the map

𝑟:ℝ2∖{0}⟶𝑆1,𝑟(𝑥)=𝑥‖𝑥‖.

Let 𝑖:𝑆1↪ℝ2∖{0} be the inclusion. Then

𝑟∘𝑖=id𝑆1⁡.

Also,

𝑖∘𝑟:ℝ2∖{0}⟶ℝ2∖{0},(𝑖∘𝑟)(𝑥)=𝑥‖𝑥‖.

Define a homotopy

𝐹:(ℝ2∖{0})×[0,1]⟶ℝ2∖{0},𝐹(𝑥,𝑡)=(1−𝑡)𝑥+𝑡𝑥‖𝑥‖.

Then 𝐹(𝑥,0)=𝑥 and 𝐹(𝑥,1)=𝑟(𝑥), so 𝐹 is a homotopy between idℝ2∖{0} and 𝑖∘𝑟. Hence 𝑟 is a homotopy equivalence, and ℝ2∖{0} has the homotopy type of 𝑆1.

Definition 1.5.3 (Deformation Retraction).

Let 𝐴⊂𝑀. A map 𝑟:𝑀→𝐴 is a retraction if 𝑟|𝐴=id𝐴, i.e. 𝑟∘𝑖=id𝐴 where 𝑖:𝐴↪𝑀 is the inclusion. It is a deformation retraction if 𝑖∘𝑟 is homotopic to id𝑀.

Proposition 1.5.1.

A deformation retraction is a homotopy equivalence.

1.5.2 The Homotopy Axiom

Theorem 1.6 (Homotopy Invariance of de Rham Cohomology).

If two smooth maps 𝑓0,𝑓1:𝑀→𝑁 are smoothly homotopic, then they induce the same map on de Rham cohomology:

𝑓∗0=𝑓∗1:𝐻∗(𝑁)⟶𝐻∗(𝑀).

Proof.

See the next section ∎

Corollary 1.6.1.

If 𝑓:𝑀→𝑁 is a homotopy equivalence, then the induced map

𝑓∗:𝐻∗(𝑁)⟶𝐻∗(𝑀)

is an isomorphism.

Proof.

Let 𝑔:𝑁→𝑀 be a homotopy inverse of 𝑓. Then 𝑔∘𝑓∼id𝑀 and 𝑓∘𝑔∼id𝑁. By the homotopy axiom,

(𝑔∘𝑓)∗=id𝐻∗(𝑀)=𝑓∗∘𝑔∗,(𝑓∘𝑔)∗=id𝐻∗(𝑁)=𝑔∗∘𝑓∗.

Thus 𝑓∗ has two-sided inverse 𝑔∗, hence is an isomorphism. ∎

Corollary 1.6.2.

Manifolds with the same homotopy type have isomorphic de Rham cohomology.

Example 1.6.1 ( Cohomology of ℝ𝑛).

Since ℝ𝑛 is contractible, it has the homotopy type of a point. Hence

𝐻𝑘(ℝ𝑛)≅{ℝ,𝑘=0,0,𝑘>0.
Example 1.6.2 ( Cohomology of a Cylinder).

The cylinder 𝐶=𝑆1×[0,1] deformation retracts onto 𝑆1. Therefore,

𝐻∗(𝐶)≅𝐻∗(𝑆1).

In particular, 𝐻1(𝐶)≅ℝ.

1.5.3 The Circle and Its Cohomology

We have already computed 𝐻∗(𝑆1) using Mayer–Vietoris:

𝐻0(𝑆1)≅ℝ,𝐻1(𝑆1)≅ℝ,𝐻𝑘(𝑆1)=0 (𝑘≥2).

A generator of 𝐻1(𝑆1) can be represented by the angular form

𝜔=−𝑦𝑑𝑥+𝑥𝑑𝑦2𝜋(𝑥2+𝑦2)=𝑑𝜃2𝜋.

Indeed,

∫𝑆1𝜔=1,

so [𝜔] is the preferred generator.

Remark 1.6.1 (Integration on a Cylinder).

Let 𝐶=𝑆1×[0,1] with boundary 𝜕𝐶=𝑆1top−𝑆1bottom. For any closed 1-form 𝜔 on 𝐶, Stokes’ theorem gives

0=∫𝐶𝑑𝜔=∫𝜕𝐶𝜔=∫𝑆1top𝜔−∫𝑆1bottom𝜔.

Thus the integral of a closed 1-form is the same on the top and bottom circles. This fact is used in the construction of the connecting homomorphism in Mayer–Vietoris for the torus.

1.5.4 Cohomology of the Torus

Let 𝑇=𝑆1×𝑆1 be the 2-torus. We compute its de Rham cohomology using the Mayer–Vietoris sequence.

Choose an open cover {𝑈,𝑉} of 𝑇 as follows. Let 𝑝,𝑞 be distinct points on 𝑆1, and set

𝑈=𝑆1×(𝑆1∖{𝑝}),𝑉=(𝑆1∖{𝑞})×𝑆1.

Then 𝑈 and 𝑉 are each homeomorphic to a cylinder 𝑆1×ℝ, so

𝐻0(𝑈)≅𝐻0(𝑉)≅ℝ,𝐻1(𝑈)≅𝐻1(𝑉)≅ℝ,𝐻𝑘(𝑈)=𝐻𝑘(𝑉)=0 (𝑘≥2).

The intersection

𝑈∩𝑉=(𝑆1∖{𝑞})×(𝑆1∖{𝑝})

is a disjoint union of two open rectangles (or equivalently, two contractible components), so

𝐻0(𝑈∩𝑉)≅ℝ⊕ℝ,𝐻1(𝑈∩𝑉)=0,𝐻𝑘(𝑈∩𝑉)=0 (𝑘≥1).

The Mayer–Vietoris sequence for this cover is:

0→𝐻0(𝑇)𝑖∗⟶𝐻0(𝑈)⊕𝐻0(𝑉)𝑗∗⟶𝐻0(𝑈∩𝑉)𝛿0⟶𝐻1(𝑇)𝑖∗⟶𝐻1(𝑈)⊕𝐻1(𝑉)𝑗∗⟶𝐻1(𝑈∩𝑉)→𝐻2(𝑇)→0.

Since 𝐻1(𝑈∩𝑉)=0, the map 𝑗∗:ℝ⊕ℝ→0 is zero, so its kernel is all of ℝ⊕ℝ. Thus Im⁡𝑖∗=ℝ2, so 𝑖∗:𝐻1(𝑇)→ℝ2 is surjective. Also, Im⁡𝛿0=ker⁡𝑖∗. We compute 𝛿0. The map 𝑗∗:ℝ2→ℝ2 (since 𝐻0(𝑈∩𝑉)≅ℝ2) sends a pair (𝛼,𝛽)∈ℝ2 (representing constant functions on U and V) to the pair of restrictions to the two components of 𝑈∩𝑉. Actually, the two components of 𝑈∩𝑉 correspond to the choices of signs; the restriction of a constant function from U and V are identical on each component, so the map is (𝛼,𝛽)↦(𝛼−𝛽,𝛼−𝛽). Its image is the diagonal {(𝑡,𝑡)}⊂ℝ2. Hence ker⁡𝛿0=Im⁡𝑗∗≅ℝ, so 𝛿0 is injective with image of dimension 1. Therefore ker⁡𝑖∗ is 1-dimensional, and since 𝑖∗ is surjective onto ℝ2, we get

𝐻1(𝑇)≅ℝ2.

For 𝐻2(𝑇), we need a cover with non-trivial first cohomology of the intersection. A standard choice is to take 𝑈 and 𝑉 as two open sets each homeomorphic to a cylinder, but with intersection homeomorphic to two disjoint cylinders, so that 𝐻1(𝑈∩𝑉)≅ℝ⊕ℝ. With such a cover, the Mayer–Vietoris sequence yields

𝐻2(𝑇)≅ℝ.

Combining, we obtain

𝐻0(𝑇)≅ℝ,𝐻1(𝑇)≅ℝ2,𝐻2(𝑇)≅ℝ,𝐻𝑘(𝑇)=0 (𝑘≥3).
Remark 1.6.2.

The computation of 𝐻2(𝑇) requires a different choice of open cover (e.g., 𝑈 and 𝑉 chosen so that 𝑈∩𝑉 is two cylinders). The details are standard and can be found in any textbook on differential topology.

Example 1.6.3 (Generators of 𝐻1(𝑇)).

On the torus, the two independent 1-forms

𝑑𝜃1,𝑑𝜃2

(where 𝜃𝑖 are the angular coordinates on each 𝑆1 factor) represent a basis of 𝐻1(𝑇). Their wedge product 𝑑𝜃1∧𝑑𝜃2 generates 𝐻2(𝑇), and

∫𝑇𝑑𝜃1∧𝑑𝜃2=(2𝜋)2.

Normalizing by (2𝜋)−2 gives the standard generator with integral 1.

Proof of the Homotopy Axiom

We now give a detailed proof of the homotopy axiom using the language of cochain complexes and chain homotopies.

Definition 1.6.1 (Cochain Homotopy).

Let

𝜑,𝜓:𝐴∙⟶𝐵∙

be cochain maps between cochain complexes. A cochain homotopy from 𝜑 to 𝜓 is a collection of linear maps

𝐾:𝐴𝑘⟶𝐵𝑘−1

such that

𝑑𝐵∘𝐾+𝐾∘𝑑𝐴=𝜓−𝜑:𝐴𝑘⟶𝐵𝑘.
Lemma 1.6.1.

If there exists a cochain homotopy 𝐾 from 𝜑 to 𝜓, then

𝜑∗=𝜓∗:𝐻𝑘(𝐴∙)⟶𝐻𝑘(𝐵∙).

Proof.

Let [𝑎]∈𝐻𝑘(𝐴∙), so 𝑑𝐴𝑎=0. Then

𝜓(𝑎)−𝜑(𝑎)=𝑑𝐵𝐾(𝑎)+𝐾𝑑𝐴(𝑎)=𝑑𝐵𝐾(𝑎).

Thus 𝜓(𝑎)−𝜑(𝑎) is exact, hence [𝜓(𝑎)]=[𝜑(𝑎)] in 𝐻𝑘(𝐵∙). ∎

Reduction to Two Inclusions

Let 𝐹:𝑁×[0,1]→𝑀 be a smooth homotopy between 𝑓0 and 𝑓1. Define inclusions

𝑗0,𝑗1:𝑁⟶𝑁×[0,1],𝑗0(𝑥)=(𝑥,0),𝑗1(𝑥)=(𝑥,1).

Then 𝑓0=𝐹∘𝑗0 and 𝑓1=𝐹∘𝑗1. By functoriality,

𝑓∗0=𝑗∗0∘𝐹∗,𝑓∗1=𝑗∗1∘𝐹∗.

It suffices to show that

𝑗∗0=𝑗∗1:𝐻𝑘(𝑁×[0,1])⟶𝐻𝑘(𝑁).

We will construct a cochain homotopy 𝐾 from 𝑗∗0 to 𝑗∗1 on the de Rham complexes:

𝐾:Ω𝑘(𝑁×[0,1])⟶Ω𝑘−1(𝑁),

such that

𝑑𝐾+𝐾𝑑=𝑗∗1−𝑗∗0.

Local Definition of 𝐾

On a coordinate chart (𝑈,𝑥1,…,𝑥𝑛) of 𝑁, a 𝑘-form on 𝑈×[0,1] is a sum of two types:

(I)𝑓(𝑥,𝑡)𝑑𝑥𝑖1∧⋯∧𝑑𝑥𝑖𝑘=:𝑓𝑑𝑥𝐼,
(II)𝑔(𝑥,𝑡)𝑑𝑡∧𝑑𝑥𝑗1∧⋯∧𝑑𝑥𝑗𝑘−1=:𝑔𝑑𝑡∧𝑑𝑥𝐽,

where 𝐼=(𝑖1,…,𝑖𝑘) and 𝐽=(𝑗1,…,𝑗𝑘−1).

Define 𝐾 locally by

𝐾(𝑓𝑑𝑥𝐼)=0,
𝐾(𝑔𝑑𝑡∧𝑑𝑥𝐽)=(∫10𝑔(𝑥,𝑡)𝑑𝑡)𝑑𝑥𝐽.

Verification of the Identity 𝑑𝐾+𝐾𝑑=𝑗∗1−𝑗∗0

We verify the identity for forms of type (I). The verification for type (II) is similar and will be omitted.

Type (I): Let 𝜔=𝑓(𝑥,𝑡)𝑑𝑥𝐼. Since 𝐾(𝜔)=0, we have

(𝑑𝐾+𝐾𝑑)(𝜔)=𝐾(𝑑𝜔).

Now

𝑑𝜔=𝑑𝑓∧𝑑𝑥𝐼=𝑛∑𝑗=1𝜕𝑓𝜕𝑥𝑗𝑑𝑥𝑗∧𝑑𝑥𝐼+𝜕𝑓𝜕𝑡𝑑𝑡∧𝑑𝑥𝐼.

The first sum contains no 𝑑𝑡 factor, hence its 𝐾-image is zero. Therefore

𝐾(𝑑𝜔)=𝐾(𝜕𝑓𝜕𝑡𝑑𝑡∧𝑑𝑥𝐼)=(∫10𝜕𝑓𝜕𝑡𝑑𝑡)𝑑𝑥𝐼=(𝑓(𝑥,1)−𝑓(𝑥,0))𝑑𝑥𝐼.

On the other hand,

(𝑗∗1−𝑗∗0)(𝜔)=𝑓(𝑥,1)𝑑𝑥𝐼−𝑓(𝑥,0)𝑑𝑥𝐼=(𝑓(𝑥,1)−𝑓(𝑥,0))𝑑𝑥𝐼.

Thus the identity holds for type (I).

Type (II): A direct computation (reordering the wedge factors so that 𝑑𝑡 appears first) shows that

(𝑑𝐾+𝐾𝑑)(𝑔𝑑𝑡∧𝑑𝑥𝐽)=0,

while (𝑗∗1−𝑗∗0)(𝑔𝑑𝑡∧𝑑𝑥𝐽)=0 because the pullback of 𝑑𝑡 under 𝑗0 and 𝑗1 is zero. Hence the identity also holds for type (II).

Coordinate Independence of 𝐾

We now prove that the local definition of 𝐾 is independent of the chosen coordinates.

Proposition 1.6.1 (Coordinate Independence of 𝐾).

Let (𝑈,𝑥1,…,𝑥𝑛) and (𝑉,𝑦1,…,𝑦𝑛) be two overlapping coordinate charts on 𝑁. For any form 𝜔∈Ω𝑘(𝑁×[0,1]), the value of 𝐾(𝜔) computed in the 𝑥-coordinates agrees with that computed in the 𝑦-coordinates on the intersection 𝑈∩𝑉.

Proof.

It suffices to consider forms of type (II), since type (I) is mapped to zero and is trivially coordinate-independent. On the overlap, write

𝜔=∑𝑗𝑓𝑗(𝑥,𝑡)𝑑𝑡∧𝑑𝑥𝐽=∑𝑖𝑔𝑖(𝑦,𝑡)𝑑𝑡∧𝑑𝑦𝐼,

where 𝐽=(𝑗1,…,𝑗𝑘−1) and 𝐼=(𝑖1,…,𝑖𝑘−1). The coordinate transformation gives

𝑑𝑦𝐼=∑𝐽𝜕𝑦𝐼𝜕𝑥𝐽𝑑𝑥𝐽,

so

∑𝑖𝑔𝑖(𝑦,𝑡)𝑑𝑡∧𝑑𝑦𝐼=∑𝑖,𝐽𝑔𝑖(𝑦,𝑡)𝜕𝑦𝐼𝜕𝑥𝐽𝑑𝑡∧𝑑𝑥𝐽.

Comparing coefficients with ∑𝑗𝑓𝑗(𝑥,𝑡)𝑑𝑡∧𝑑𝑥𝐽, we obtain

𝑓𝑗(𝑥,𝑡)=∑𝑖𝑔𝑖(𝑦(𝑥),𝑡)𝜕𝑦𝐼𝜕𝑥𝐽.

Now, in the 𝑥-coordinates,

𝐾𝑥(𝜔)=∑𝑗(∫10𝑓𝑗(𝑥,𝑡)𝑑𝑡)𝑑𝑥𝐽,

while in the 𝑦-coordinates,

𝐾𝑦(𝜔)=∑𝑖(∫10𝑔𝑖(𝑦,𝑡)𝑑𝑡)𝑑𝑦𝐼.

Using the relation between 𝑓𝑗 and 𝑔𝑖, we have

𝐾𝑥(𝜔)=∑𝑗(∫10∑𝑖𝑔𝑖(𝑦(𝑥),𝑡)𝜕𝑦𝐼𝜕𝑥𝐽𝑑𝑡)𝑑𝑥𝐽=∑𝑖(∫10𝑔𝑖(𝑦(𝑥),𝑡)𝑑𝑡)∑𝐽𝜕𝑦𝐼𝜕𝑥𝐽𝑑𝑥𝐽=∑𝑖(∫10𝑔𝑖(𝑦(𝑥),𝑡)𝑑𝑡)𝑑𝑦𝐼=𝐾𝑦(𝜔).

Thus the two expressions agree on 𝑈∩𝑉. ∎

The coordinate independence allows us to patch the local definitions of 𝐾 together using a partition of unity (or simply by defining 𝐾(𝜔) on each chart and gluing). Hence we obtain a global operator

𝐾:Ω𝑘(𝑁×[0,1])⟶Ω𝑘−1(𝑁).

Since the identity 𝑑𝐾+𝐾𝑑=𝑗∗1−𝑗∗0 is local, and we have verified it on each chart, it holds globally. Therefore 𝐾 is a cochain homotopy from 𝑗∗0 to 𝑗∗1. By the lemma, 𝑗∗0=𝑗∗1 on cohomology. Consequently,

𝑓∗0=𝑗∗0∘𝐹∗=𝑗∗1∘𝐹∗=𝑓∗1,

which proves the homotopy axiom.