Interior Product: Definition & Understanding

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    Interior Product
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SUMMARY

The interior product is mathematically defined as ##i_X:\Omega^r(M)\to \Omega^{r-1}(M)##, where X represents a vector on the manifold and ##\Omega^r(M)## denotes the vector space of r-forms at a point p on the manifold. The operation of the interior product on an r-form ##\omega \in \Omega^r(M)## is expressed as ##(i_X(\omega))(X_1,\ldots ,X_{r-1}) := \omega(X,X_1,\ldots ,X_{r-1})##. This indicates that while ##i_X## transforms an r-form into an r-1 form, it requires an additional argument from the vector X, clarifying the apparent contradiction in its definition.

PREREQUISITES
  • Understanding of differential forms and their notation, specifically ##\Omega^r(M)##.
  • Familiarity with vector fields and their roles in manifold theory.
  • Knowledge of the properties and operations of the interior product in differential geometry.
  • Basic comprehension of manifolds and their dimensionality.
NEXT STEPS
  • Study the properties of differential forms in the context of manifold theory.
  • Learn about the applications of the interior product in various fields of mathematics.
  • Explore the relationship between the exterior derivative and the interior product.
  • Investigate examples of interior products in specific manifolds to solidify understanding.
USEFUL FOR

Mathematicians, students of differential geometry, and anyone interested in the applications of differential forms and the interior product in advanced mathematical contexts.

Silviu
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Hello! The interior product is defined as ##i_X:\Omega^r(M)\to \Omega^{r-1}(M)##, with X being a vector on the manifold and ##\Omega^r(M)## the vector space of r-form at a point p on the manifold. Now for ##\omega \in \Omega^r(M) ## we have ##i_X\omega(X_1, ... X_{r-1}) = \omega (X,X_1, ... X_{r-1})##. I am not sure I understand it. Based on this definition, ##i_X## acts on an r-1 form and it turns it into an r-form, by making it acts on X, too. But by the definition in the first line, ##i_X## should act the other way around. What am I reading wrong here? Thank you!
 
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There is no contradiction. Say ##\omega \in \Omega^r(M)##. Then ##\omega## applies to ##r## vector fields. Now we want to define ##i_X(\omega) \in \Omega^{r-1}(M)##, i.e. by its action on ##r-1## vector fields ##X_1,\ldots , X_{r-1}##. We do this by ##(i_X(\omega))(X_1,\ldots ,X_{r-1}) := \omega(X,X_1,\ldots ,X_{r-1})##.
 
To put it slightly differently, ##i_X\omega## is an ##r-1##-form so it takes ##r-1## arguments as you can see on the LHS of your expression. On the RHS of the expression you have only ##\omega##, which is an ##r#-form and therefore takes ##r## arguments. Clearly, there are ##r-1## ##X_i## on the LHS and the RHS therefore needs the extra argument ##X##, which is the ##X## of the interior product.
 

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