Interior products: Difference between revisions

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(Created page with "The left and right ''interior products'' are special products in geometric algebra that are useful for performing projections. These products cancel common factors in their operands and thus reduce grade. Depending on the choice of dualization function, there are several possible interior products. We define the interior products in terms of the left and right complements. Interior products are also known as contraction products. == Left and Right Interior Prod...")
 
 
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The left and right ''interior products'' are special products in geometric algebra that are useful for performing [[projections]]. These products cancel common factors in their operands and thus reduce grade. Depending on the choice of dualization function, there are several possible interior products. We define the interior products in terms of the left and right [[complements]].
The ''interior products'' are special products in geometric algebra that are useful for a number of operations including [[projections]]. They are defined as the [[wedge product]] or [[antiwedge product]] between one object and either the [[bulk dual]] or [[weight dual]] of another object.


Interior products are also known as contraction products.
== Contractions ==


== Left and Right Interior Products ==
The ''bulk contraction'' between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as


The ''left interior product'' between elements $$\mathbf a$$ and $$\mathbf b$$ is written as $$\mathbf a \mathbin{\unicode{x22A3}} \mathbf b$$ and defined as
:$$\mathrm{bulk\ contraction}(\mathbf a, \mathbf b) = \mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605}$$ .


:$$\mathbf a \mathbin{\unicode{x22A3}} \mathbf b = \underline{\mathbf a} \vee \mathbf b$$ .
The ''weight contraction'' between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as


The ''right interior product'' between elements $$\mathbf a$$ and $$\mathbf b$$ is written as $$\mathbf a \mathbin{\unicode{x22A2}} \mathbf b$$ and defined as
:$$\mathrm{weight\ contraction}(\mathbf a, \mathbf b) = \mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606}$$ .


:$$\mathbf a \mathbin{\unicode{x22A2}} \mathbf b = \mathbf a \vee \overline{\mathbf b}$$ .
The contractions have the effect of subtracting grades so that


The left and right interior products satisfy the relationship
:$$\operatorname{gr}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605}) = \operatorname{gr}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606}) = \operatorname{gr}(\mathbf a) - \operatorname{gr}(\mathbf b)$$ .


:$$\mathbf a \mathbin{\unicode{x22A3}} \mathbf b = (-1)^{\operatorname{gr}(\mathbf a)\left[\operatorname{gr}(\mathbf a) + \operatorname{gr}(\mathbf b)\right]}\mathbf b \mathbin{\unicode{x22A2}} \mathbf a$$ .
In the case that the grades of $$\mathbf a$$ and $$\mathbf b$$ are the same, the bulk and weight contractions are equal to dot products written as


The following Cayley table shows the interior products between all pairs of basis elements in the 4D rigid geometric algebra $$\mathcal G_{3,0,1}$$. Cells colored blue belong only to the left interior product and are zero for the right interior product. Cells colored red belong only to the right interior product and are zero for the left interior product. Cells colored purple along the diagonal belong to both the left and right interior products.
:$$\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605} = \mathbf a \mathbin{\unicode["segoe ui symbol"]{x2022}} \mathbf b$$


and


[[Image:InteriorProduct.svg|720px]]
:$$\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606} = (\mathbf a \mathbin{\unicode["segoe ui symbol"]{x2218}} \mathbf b) \vee \mathbf 1$$ .


== Left and Right Interior Antiproducts ==
The bulk contraction satisfies the identity


Like all operations in geometric algebra, the interior products have duals, which we call ''interior antiproducts''. The right and left interior antiproducts between elements $$\mathbf a$$ and $$\mathbf b$$ are written as $$\mathbf a \mathbin{\unicode{x22A8}} \mathbf b$$ and $$\mathbf a \mathbin{\unicode{x2AE4}} \mathbf b$$, respectively, and they are defined as follows.
:$$\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605} = \langle\mathbf{\tilde b} \mathbin{\unicode{x27D1}} \mathbf a\rangle_{\operatorname{gr}(\mathbf a) - \operatorname{gr}(\mathbf b)}$$ .


:$$\mathbf a \mathbin{\unicode{x22A8}} \mathbf b = \overline{\underline{\mathbf a} \mathbin{\unicode{x22A2}} \underline{\mathbf b}} = \mathbf a \wedge \overline{\mathbf b}$$
The following Cayley table shows the bulk and weight contraction products between all pairs of basis elements in the 4D rigid geometric algebra $$\mathcal G_{3,0,1}$$. The values of the bulk contraction are highlighted in green, and the values of the weight contraction are highlighted in purple. The darker green cells along the diagonal correspond to the nonzero entries of the metric $$\mathbf G$$.


:$$\mathbf a \mathbin{\unicode{x2AE4}} \mathbf b = \overline{\underline{\mathbf a} \mathbin{\unicode{x22A3}} \underline{\mathbf b}} = \underline{\mathbf a} \wedge \mathbf b$$


The interior antiproducts are also related to the opposite interior products through the following equalities.
[[Image:Constractions.svg|720px]]


:$$\mathbf a \mathbin{\unicode{x22A8}} \mathbf b = \overline{\mathbf a \mathbin{\unicode{x22A3}} \mathbf b}$$
== Expansions ==


:$$\mathbf a \mathbin{\unicode{x2AE4}} \mathbf b = \underline{\mathbf a \mathbin{\unicode{x22A2}} \mathbf b}$$
The ''bulk expansion'' between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as


The following Cayley table shows the interior antiproducts between all pairs of basis elements in the 4D rigid geometric algebra $$\mathcal G_{3,0,1}$$. Cells colored blue belong only to the left interior antiproduct and are zero for the right interior antiproduct. Cells colored red belong only to the right interior antiproduct and are zero for the left interior antiproduct. Cells colored purple along the diagonal belong to both the left and right interior antiproducts.
:$$\mathrm{bulk\ expansion}(\mathbf a, \mathbf b) = \mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2605}$$ .


The ''weight expansion'' between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as


[[Image:InteriorAntiproduct.svg|720px]]
:$$\mathrm{weight\ expansion}(\mathbf a, \mathbf b) = \mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2606}$$ .
 
The expansions have the effect of subtracting antigrades so that
 
:$$\operatorname{ag}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605}) = \operatorname{ag}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606}) = \operatorname{ag}(\mathbf a) - \operatorname{ag}(\mathbf b)$$ .
 
In the case that the grades (and thus antigrades) of $$\mathbf a$$ and $$\mathbf b$$ are the same, the bulk and weight expansions are equal to dot products written as
 
:$$\mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2606} = \mathbf a \mathbin{\unicode["segoe ui symbol"]{x2218}} \mathbf b$$
 
and
 
:$$\mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2605} = (\mathbf a \mathbin{\unicode["segoe ui symbol"]{x2022}} \mathbf b) \wedge \mathbf {\large\unicode{x1D7D9}}$$ .
 
The weight expansion satisfies the identity
 
:$$\mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2606} = \langle\!\langle\smash{\mathbf{\underset{\Large\unicode{x7E}}{b}}} \mathbin{\unicode{x27C7}} \mathbf a\rangle\!\rangle_{\operatorname{ag}(\mathbf a) - \operatorname{ag}(\mathbf b)}$$ .
 
The following Cayley table shows the bulk and weight expansion products between all pairs of basis elements in the 4D rigid geometric algebra $$\mathcal G_{3,0,1}$$. The values of the bulk expansion are highlighted in green, and the values of the weight expansion are highlighted in purple. The darker purple cells along the diagonal correspond to the nonzero entries of the antimetric $$\mathbb G$$.
 
 
[[Image:Expansions.svg|720px]]
 
== In the Book ==
 
* Interior products, contractions, and expansions are discussed in Section 2.13.


== See Also ==
== See Also ==


* [[Projections]]
* [[Projections]]

Latest revision as of 03:13, 22 August 2024

The interior products are special products in geometric algebra that are useful for a number of operations including projections. They are defined as the wedge product or antiwedge product between one object and either the bulk dual or weight dual of another object.

Contractions

The bulk contraction between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as

$$\mathrm{bulk\ contraction}(\mathbf a, \mathbf b) = \mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605}$$ .

The weight contraction between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as

$$\mathrm{weight\ contraction}(\mathbf a, \mathbf b) = \mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606}$$ .

The contractions have the effect of subtracting grades so that

$$\operatorname{gr}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605}) = \operatorname{gr}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606}) = \operatorname{gr}(\mathbf a) - \operatorname{gr}(\mathbf b)$$ .

In the case that the grades of $$\mathbf a$$ and $$\mathbf b$$ are the same, the bulk and weight contractions are equal to dot products written as

$$\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605} = \mathbf a \mathbin{\unicode["segoe ui symbol"]{x2022}} \mathbf b$$

and

$$\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606} = (\mathbf a \mathbin{\unicode["segoe ui symbol"]{x2218}} \mathbf b) \vee \mathbf 1$$ .

The bulk contraction satisfies the identity

$$\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605} = \langle\mathbf{\tilde b} \mathbin{\unicode{x27D1}} \mathbf a\rangle_{\operatorname{gr}(\mathbf a) - \operatorname{gr}(\mathbf b)}$$ .

The following Cayley table shows the bulk and weight contraction products between all pairs of basis elements in the 4D rigid geometric algebra $$\mathcal G_{3,0,1}$$. The values of the bulk contraction are highlighted in green, and the values of the weight contraction are highlighted in purple. The darker green cells along the diagonal correspond to the nonzero entries of the metric $$\mathbf G$$.


Expansions

The bulk expansion between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as

$$\mathrm{bulk\ expansion}(\mathbf a, \mathbf b) = \mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2605}$$ .

The weight expansion between elements $$\mathbf a$$ and $$\mathbf b$$ is defined as

$$\mathrm{weight\ expansion}(\mathbf a, \mathbf b) = \mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2606}$$ .

The expansions have the effect of subtracting antigrades so that

$$\operatorname{ag}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2605}) = \operatorname{ag}(\mathbf a \vee \mathbf b^\unicode["segoe ui symbol"]{x2606}) = \operatorname{ag}(\mathbf a) - \operatorname{ag}(\mathbf b)$$ .

In the case that the grades (and thus antigrades) of $$\mathbf a$$ and $$\mathbf b$$ are the same, the bulk and weight expansions are equal to dot products written as

$$\mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2606} = \mathbf a \mathbin{\unicode["segoe ui symbol"]{x2218}} \mathbf b$$

and

$$\mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2605} = (\mathbf a \mathbin{\unicode["segoe ui symbol"]{x2022}} \mathbf b) \wedge \mathbf {\large\unicode{x1D7D9}}$$ .

The weight expansion satisfies the identity

$$\mathbf a \wedge \mathbf b^\unicode["segoe ui symbol"]{x2606} = \langle\!\langle\smash{\mathbf{\underset{\Large\unicode{x7E}}{b}}} \mathbin{\unicode{x27C7}} \mathbf a\rangle\!\rangle_{\operatorname{ag}(\mathbf a) - \operatorname{ag}(\mathbf b)}$$ .

The following Cayley table shows the bulk and weight expansion products between all pairs of basis elements in the 4D rigid geometric algebra $$\mathcal G_{3,0,1}$$. The values of the bulk expansion are highlighted in green, and the values of the weight expansion are highlighted in purple. The darker purple cells along the diagonal correspond to the nonzero entries of the antimetric $$\mathbb G$$.


In the Book

  • Interior products, contractions, and expansions are discussed in Section 2.13.

See Also