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Grassmann Algebra

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TheComplement.nb 22<br />

We can transform the columns of basis elements in this equation into the form of the preceding<br />

one with the transformation T which is simply determined as:<br />

� 0 0 1<br />

�������<br />

��������<br />

T � 0 �1 0<br />

� 1 0 0�<br />

;<br />

��������<br />

T�<br />

�<br />

e1 � e2<br />

e1 � e3<br />

e2 � e3<br />

��������<br />

�<br />

�<br />

� e2 � e3<br />

�������<br />

��������<br />

� e3<br />

�������<br />

��������<br />

��e1 � e3� ; T��e2<br />

� e1 � e2 � � e1 �<br />

�<br />

��������<br />

�<br />

And since this transformation is its own inverse, we can also transform G2 to T G2�T. We now<br />

expect this transformed array to be the array of cofactors of the metric tensor G1 . We can easily<br />

check this in Mathematica by entering the predicate<br />

e1<br />

e2<br />

e3<br />

��������<br />

�<br />

;<br />

Simplify�G1.�T.G2.T� � Det�G1��IdentityMatrix�3��<br />

True<br />

� Creating tables of induced metrics<br />

You can create a table of all the induced metrics by declaring a metric and then entering<br />

MetricTable.<br />

2001 4 5<br />

�3; M� ��1, 0, Ν�, �0, �1, 0�, �Ν, 0,�1��;<br />

DeclareMetric�M�; MetricTable<br />

� METRIC<br />

� 0<br />

� l<br />

� 2<br />

� 3<br />

1<br />

� 1<br />

�������<br />

0<br />

� Ν<br />

0<br />

�1<br />

0<br />

Ν ��������<br />

0<br />

�1 �<br />

� �1<br />

��������<br />

0<br />

�<br />

0<br />

�1 �Ν<br />

Ν<br />

2 Ν 0<br />

���������<br />

0<br />

1�<br />

1 �Ν 2

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