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Grassmann Algebra

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ExpTheGeneralizedProduct.nb 6<br />

Α m ���� Β j<br />

Λ<br />

� m<br />

Λ �<br />

� �<br />

i�1<br />

�Α i<br />

Λ<br />

���� Βj��Α<br />

Λ<br />

i<br />

m�Λ<br />

Substituting this in the above expression for the generalized product gives:<br />

Α m ����� Λ �Β k<br />

�������������<br />

Λ<br />

� � �<br />

i�1<br />

j�1<br />

�<br />

�<br />

� k<br />

Λ �<br />

� m<br />

�Α i<br />

Λ<br />

���� Βj��Α<br />

Λ<br />

i<br />

�������������<br />

� Β<br />

m�Λ<br />

�<br />

j<br />

k�Λ<br />

The expansion of the generalized product in terms of both factors Α m and Β k<br />

Α m ����� Λ �Β k<br />

Α m � Α 1<br />

Λ<br />

� m<br />

Λ �<br />

� �<br />

� Α1<br />

m�Λ<br />

i�1<br />

� k<br />

Λ �<br />

�<br />

j�1<br />

� Α2<br />

Λ<br />

�Α i<br />

Λ<br />

���� Βj�<br />

Α<br />

Λ<br />

i<br />

� Βj<br />

m�Λ k�Λ<br />

� Α2<br />

m�Λ � �, Β k<br />

� Β 1<br />

Λ<br />

0 �Λ�Min�m, k�<br />

� Β 1<br />

k�Λ<br />

� Β 2<br />

Λ<br />

The quasi-commutativity of the generalized product<br />

is thus given by:<br />

� Β2 � �<br />

k�Λ<br />

From the symmetric form of the generalized product [10.8] we can show directly that the<br />

ordering of the factors in a product is immaterial except perhaps for a sign.<br />

To show this we begin with the symmetric form [10.8], and rewrite it for the product of Β k<br />

Α, that is, Β����� �Α . We then reverse the order of the exterior product to obtain the terms of Α����� �Β<br />

m k Λ m m Λ k<br />

except for possibly a sign. The inner product is of course symmetric, and so can be written in<br />

either ordering.<br />

�<br />

����� �Α � �<br />

Λ m k<br />

Λ � �<br />

��<br />

m<br />

Λ �<br />

Β k<br />

� k<br />

Λ �<br />

� m<br />

Λ �<br />

� ���<br />

j�1 i�1<br />

j�1<br />

�Α i<br />

Λ<br />

i�1<br />

�Β j<br />

Λ<br />

Comparison with [10.8] then gives:<br />

2001 4 26<br />

���� Αi� Βj � Α<br />

Λ k�Λ<br />

i<br />

m�Λ<br />

���� Βj���1�<br />

Λ<br />

�m�Λ���k�Λ� �Α i<br />

� Βj<br />

m�Λ k�Λ<br />

Α m ����� Λ �Β k<br />

� ��1� �m�Λ���k�Λ� �Β����� �Α<br />

k Λ m<br />

10.8<br />

with<br />

10.9

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