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Grassmann Algebra

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ExpTheGeneralizedProduct.nb 34<br />

Flatten�<br />

Table�ToScalarProducts� ����Α<br />

�<br />

� �������� � � ��1�<br />

�m<br />

p�<br />

Λ k<br />

m Λ �Α �<br />

m ����Γ<br />

�<br />

����� ���� ��.<br />

�p<br />

Λ k�<br />

OrthogonalSimplificationRules���Α, Β���, m k<br />

�m, 0, 2�, �k, 0, m�, �p, 0, m�, �Λ, 0,Min�k, p����<br />

�0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0�<br />

10.14 The Generalized Product of Intersecting<br />

Orthogonal Elements<br />

The case Λ < p<br />

Consider three simple elements Α, Β and Γ . The elements Γ � Α and Γ � Β may then be<br />

m k p<br />

p m p k<br />

considered elements with an intersection Γ. As has been shown in Section 10.12, generalized<br />

p<br />

products of such intersecting elements are zero whenever the grade Λ of the product is less than<br />

the grade of the intersection. Hence the product will be zero for Λ < p, independent of the<br />

orthogonality relationships of its factors.<br />

� The case Λ ≥ p<br />

Consider now the case of three simple elements Α, Β and Γ where Γ is totally orthogonal to<br />

m k p p<br />

both Α and Β (and hence to Α � Β). A simple element Γ is totally orthogonal to an element Α if<br />

m k<br />

m k<br />

p<br />

m<br />

and only if Α ���� Γi � 0 for all Γi belonging to Γ. m p<br />

The generalized product of the elements Γ � Α and Γ � Β<br />

p m p k<br />

of order Λ ≥ p is a scalar factor Γ ���� Γ<br />

p p<br />

times the generalized product of the factors Α and Β, but of an order lower by the grade of the<br />

m k<br />

common factor; that is, of order Λ–p.<br />

Γ p<br />

����Γ<br />

�<br />

� Α�������� �<br />

�p<br />

m�<br />

Λ �<br />

�<br />

�Γ1� Γ2 � � � Γp<br />

Note here that the factors of Γ p<br />

factors of Α. Nor the factors of Β. m k<br />

���à p<br />

�<br />

� ��� �<br />

k�<br />

�<br />

�<br />

���à p<br />

�<br />

���� Γ�����Α� ���� �Β� p�<br />

m Λ�p k<br />

���� Γi � 0 Λ�p<br />

Α m ���� Γi �Β k<br />

are not necessarily orthogonal to each other. Neither are the<br />

We can test this out by making a table of cases. Here we look at the first 25 cases.<br />

2001 4 26<br />

10.39

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