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Grassmann Algebra

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ExploringHypercomplex<strong>Algebra</strong>.nb 14<br />

A ���� A � �Α �Β����� �Α �Β� �Α����Α �Α���� Β �Β���� Α �Β����Β m k m k m m m k k m k k<br />

We would like the norm of a general <strong>Grassmann</strong> number to be a scalar quantity. But<br />

none of the generalized product components of Α ����Β or Β����Α can be scalar if m and k<br />

m k k m<br />

are different, so we choose to make Β ����Α equal to - Α���� Β as a fundamental defining<br />

k m m k<br />

axiom of the hypercomplex product, thus eliminating both products from the<br />

expression for the norm. This requirement of skew-symmetry can always be satisfied<br />

because, since the grades are different, the two products are always distinguishable.<br />

Α m ���� Β k<br />

��Β���� Α<br />

k m<br />

The norm of a <strong>Grassmann</strong> number in terms of hypercomplex<br />

products<br />

More generally, suppose A were the sum of several elements of different grade.<br />

A �Α� Β �Γ� …<br />

m k p<br />

The skew-symmetry axiom then allows us to write A����A as the sum of hypercomplex<br />

squares of the components of different grade of A.<br />

A ���� A � ����Α<br />

� Β �Γ� …<br />

�m<br />

k p<br />

����<br />

����<br />

�<br />

����Α<br />

� Β �Γ<br />

�m<br />

k p<br />

And hence the norm is expressed simply as<br />

��X� � a2 �Α���� Α �Β���� Β �Γ����Γ � …<br />

m m k k p p<br />

��a �Α� Β �Γ<br />

m k p<br />

� … ����<br />

�Α����Α �Β���� Β �Γ���� Γ � …<br />

� m m k k p p<br />

� …� � a 2 �Α���� Α �Β����Β �Γ����Γ � …<br />

m m k k p p<br />

The norm of a <strong>Grassmann</strong> number of simple components<br />

Consider a <strong>Grassmann</strong> number A in which the elements Α, Β, … of each grade are<br />

m k<br />

simple.<br />

11.29<br />

11.30<br />

A �Α� Β �Γ� …<br />

m k p<br />

Then by 11.28 and 11.30 we have that the norm of A is positive and may be written as<br />

the sum of interior products of the individual simple elements.<br />

2001 4 26

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