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Grassmann Algebra

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Exploring<strong>Grassmann</strong><strong>Algebra</strong>.nb 16<br />

However, in the general case an even soul will not be nilpotent, but its powers will become zero<br />

when the grades of the terms in the power expansion exceed the dimension of the space. We can<br />

show this by calculating the powers of an even soul in spaces of successively higher<br />

dimensions. Let<br />

Zes � m � p � q � r � s � t � u � v � w � x � y � z;<br />

Table���n; Dimension, ��Zes � Zes��, �n, 3, 8�� �� TableForm<br />

3 0<br />

4 0<br />

5 0<br />

6 2 m� p � q � r � s � t<br />

7 2 m� p � q � r � s � t<br />

8 2 m� p � q � r � s � t � 2m� p � u � v � w � x � y � z<br />

� Powers of odd <strong>Grassmann</strong> numbers<br />

Odd <strong>Grassmann</strong> numbers are nilpotent. Hence all positive integer powers except the first are<br />

zero.<br />

Xo � OddGrade�X�<br />

e1 Ξ1 � e2 Ξ2 � e3 Ξ3 �Ξ7 e1 � e2 � e3<br />

��Xo � Xo�<br />

0<br />

� Computing positive powers of <strong>Grassmann</strong> numbers<br />

We can make use of the nilpotence of the odd component to compute powers of <strong>Grassmann</strong><br />

numbers more efficiently than the direct approach described at the beginning of this section by<br />

noting that it will cause a binomial expansion of the sum of the even and odd components to<br />

terminate after the first two terms. Let X � Xe � Xo , then:<br />

X p � �Xe � Xo� p � Xe p � pXe p�1 � Xo � �<br />

X p � Xe p�1 ��Xe � pXo�<br />

where the powers of p and pÐ1 refer to the exterior powers of the <strong>Grassmann</strong> numbers. For<br />

example, the cube of a general <strong>Grassmann</strong> number X in 3-space may then be calculated as<br />

2001 4 5<br />

�3; Xe � EvenGrade�X�; Xo � OddGrade�X�; ��Xe � Xe ��Xe � 3�Xo��<br />

9.1<br />

Ξ 0 3 � 3e1 Ξ 0 2 Ξ1 � 3e2 Ξ 0 2 Ξ2 � 3e3 Ξ 0 2 Ξ3 � 3 Ξ 0 2 Ξ4 e1 � e2 � 3 Ξ 0 2 Ξ5 e1 � e3 �<br />

3 Ξ 0 2 Ξ6 e2 � e3 � �Ξ0 ��6 Ξ2 Ξ5 � 6 �Ξ3 Ξ4 �Ξ1 Ξ6�� � 3 Ξ 0 2 Ξ7� e1 � e2 � e3

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