I found this statement in Raoul Bott "Differential Forms in Algebraic Topology": "Because the wedge product is an antiderivation, it descends to cohomology." Apparently this meant to be really obvious but I'm not sure how. So I thought of showing that for given $\omega, \omega_0 \in \Omega^p(M), \tau, \tau_0 \in \Omega^q(M)$ and $\omega_1 \in \Omega^{p-1}(M), \tau_1 \in \Omega^{q - 1}(M)$ such that $\omega = \omega_0 + d\omega_1, \tau = \tau_0 + d\tau_1$ then $\omega \wedge \tau = \omega_0 \wedge \tau_0 + d(\mbox{something...})$, but LHS is \begin{eqnarray} \omega \wedge \tau &=& \omega_0 \wedge \tau_0 + \omega_0 \wedge d\tau_1 + d\omega_1 \wedge \tau_0 + d\omega_1 \wedge d\tau_1 \\ &=& \omega_0 \wedge \tau_0 + \omega_0 \wedge d\tau_1 + d\omega_1 \wedge \tau_0 + d(\omega_1 \wedge d\tau_1) - (-1)^{p-1}\omega_1\wedge d^2\tau_1 \\ &=& \omega_0 \wedge \tau_0 + \omega_0 \wedge d\tau_1 + d\omega_1 \wedge \tau_0 + d(\omega_1 \wedge d\tau_1) \end{eqnarray} But I don't know how to put the rest in the total differential form. Am I even trying to show the right thing?
2026-03-26 06:30:52.1774506652
Wedge product descend to the cohomology
1k Views Asked by Bumbble Comm https://math.techqa.club/user/bumbble-comm/detail At
1
There are 1 best solutions below
Related Questions in HOMOLOGY-COHOMOLOGY
- Are these cycles boundaries?
- Cohomology groups of a torus minus a finite number of disjoint open disks
- $f$ - odd implies $d(f)$ - odd, question to the proof
- Poincarè duals in complex projective space and homotopy
- understanding proof of excision theorem
- proof of excision theorem: commutativity of a diagram
- exact sequence of reduced homology groups
- Doubts about computation of the homology of $\Bbb RP^2$ in Vick's *Homology Theory*
- the quotien space of $ S^1\times S^1$
- Rational points on conics over fields of dimension 1
Related Questions in DIFFERENTIAL-FORMS
- Using the calculus of one forms prove this identity
- Relation between Fubini-Study metric and curvature
- Integration of one-form
- Time derivative of a pullback of a time-dependent 2-form
- Elliptic Curve and Differential Form Determine Weierstrass Equation
- I want the pullback of a non-closed 1-form to be closed. Is that possible?
- How to find 1-form for Stokes' Theorem?
- Verify the statement about external derivative.
- Understanding time-dependent forms
- form value on a vector field
Related Questions in EXTERIOR-ALGEBRA
- Does curl vector influence the final destination of a particle?
- How to get the missing brick of the proof $A \circ P_\sigma = P_\sigma \circ A$ using permutations?
- Is the exterior/wedge product of differential forms injective?
- trace of exterior product of a skew matrix $M$, $\bigwedge^kM$
- Question about notation in differential forms.
- A confusing formula in Clifford algebra
- Is there a non-degenerate solution for this PDE on $\mathbb{R}^3$?
- Using the 'wedge product'
- Does every connection admit a parallel volume form?
- Derivation of Green's theorem - I have wrong negative sign
Trending Questions
- Induction on the number of equations
- How to convince a math teacher of this simple and obvious fact?
- Find $E[XY|Y+Z=1 ]$
- Refuting the Anti-Cantor Cranks
- What are imaginary numbers?
- Determine the adjoint of $\tilde Q(x)$ for $\tilde Q(x)u:=(Qu)(x)$ where $Q:U→L^2(Ω,ℝ^d$ is a Hilbert-Schmidt operator and $U$ is a Hilbert space
- Why does this innovative method of subtraction from a third grader always work?
- How do we know that the number $1$ is not equal to the number $-1$?
- What are the Implications of having VΩ as a model for a theory?
- Defining a Galois Field based on primitive element versus polynomial?
- Can't find the relationship between two columns of numbers. Please Help
- Is computer science a branch of mathematics?
- Is there a bijection of $\mathbb{R}^n$ with itself such that the forward map is connected but the inverse is not?
- Identification of a quadrilateral as a trapezoid, rectangle, or square
- Generator of inertia group in function field extension
Popular # Hahtags
second-order-logic
numerical-methods
puzzle
logic
probability
number-theory
winding-number
real-analysis
integration
calculus
complex-analysis
sequences-and-series
proof-writing
set-theory
functions
homotopy-theory
elementary-number-theory
ordinary-differential-equations
circles
derivatives
game-theory
definite-integrals
elementary-set-theory
limits
multivariable-calculus
geometry
algebraic-number-theory
proof-verification
partial-derivative
algebra-precalculus
Popular Questions
- What is the integral of 1/x?
- How many squares actually ARE in this picture? Is this a trick question with no right answer?
- Is a matrix multiplied with its transpose something special?
- What is the difference between independent and mutually exclusive events?
- Visually stunning math concepts which are easy to explain
- taylor series of $\ln(1+x)$?
- How to tell if a set of vectors spans a space?
- Calculus question taking derivative to find horizontal tangent line
- How to determine if a function is one-to-one?
- Determine if vectors are linearly independent
- What does it mean to have a determinant equal to zero?
- Is this Batman equation for real?
- How to find perpendicular vector to another vector?
- How to find mean and median from histogram
- How many sides does a circle have?
If $\omega$ and $\tau$ are closed forms (which you have not used), then
$$d(\omega \wedge \tau) = d\omega \wedge \tau + (-1)^{p-1}\omega \wedge d\tau = 0,$$
hence $\omega \wedge \tau$ is also closed, hence it corresponds to a class in cohomology. Let us see that this class depends only on the classes of $\omega$ and $\tau$. Let us suppose that $\omega = d\eta$ is exact, so that its cohomology class is trivial, and let us show that the cohomology class of $\omega \wedge \eta$ is also trivial. We have:
$$d\eta \wedge \tau = d(\eta \wedge \tau) - (-1)^{p-1}\eta \wedge d\tau$$
$$ = d(\eta \wedge \tau)$$
is also exact.