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Grassmann Algebra

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TheComplement.nb 41<br />

e i<br />

m<br />

�����<br />

i � ej � e<br />

m m<br />

In � 1 these reduce to:<br />

ei<br />

m<br />

jk ����� i<br />

��gm �ek�<br />

� e<br />

m m<br />

�<br />

����� m<br />

ej � gij� 1<br />

m<br />

�����<br />

ei � e j<br />

����� j �����<br />

�∆i� 1<br />

ei � ej<br />

����� � gij� 1<br />

�����<br />

� gm jk<br />

�� �����<br />

The regressive product of basis elements<br />

g ��ek ij<br />

� gm � 1<br />

����� m<br />

�����<br />

e i<br />

m<br />

����� m<br />

� g ij<br />

� 1<br />

�����<br />

� ej<br />

m<br />

e i � ej<br />

����� i �����<br />

�∆j� 1<br />

e i � e j<br />

����� � g ij � 1<br />

�����<br />

In the series of formulae below we have repeated the formulae derived for the exterior product<br />

and shown its equivalent for the regressive product in the same box for comparison. We have<br />

used the fact that ∆ j i and g m ij<br />

are symmetric to interchange the indices.<br />

ei<br />

m<br />

e i<br />

m<br />

ei<br />

m<br />

e i<br />

m<br />

� ej �����<br />

j �����<br />

�∆i�<br />

1<br />

m<br />

����� i �����<br />

� ej �∆j� 1<br />

m<br />

����� m<br />

� ej � gij� 1<br />

m<br />

�����<br />

����� m<br />

� g ij<br />

� 1<br />

�����<br />

� ej<br />

m<br />

The complement of a simple element is simple<br />

ei<br />

m<br />

e i<br />

m<br />

ei<br />

m<br />

e i<br />

m<br />

� ej �����<br />

j<br />

�∆i<br />

m<br />

����� i<br />

� ej �∆j<br />

m<br />

����� m<br />

� ej � gij m<br />

����� m<br />

� ej � g<br />

m<br />

ij<br />

The expression of the complement of a basis element in terms of its cobasis element in the<br />

reciprocal basis allows us a straightforward proof that the complement of a simple element is<br />

simple.<br />

To show this, suppose a simple element Α m expressed in terms of its factors Αi .<br />

2001 4 5<br />

5.65<br />

5.66<br />

5.67<br />

5.68<br />

5.69<br />

5.70<br />

5.71

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