yifli
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Given two orthonormal bases v_1,v_2,\cdots,v_n and u_1,u_2,\cdots,u_n for a vector space V, we know the following formula holds for an alternating tensor f:
f(u_1,u_2,\cdots,u_n)=\det(A)f(v_1,v_2,\cdots,v_n)
where A is the orthogonal matrix that changes one orthonormal basis to another orthonormal basis.
The volume element is the unique f such that f(v_1,v_2,\cdots,v_n)=1 for any orthonormal basis v_1,v_2,\cdots,v_n given an orientation for V.
Here is my question:
If \det(A)=-1, then f(u_1,u_2,\cdots,u_n)=-1, which makes f not unique
f(u_1,u_2,\cdots,u_n)=\det(A)f(v_1,v_2,\cdots,v_n)
where A is the orthogonal matrix that changes one orthonormal basis to another orthonormal basis.
The volume element is the unique f such that f(v_1,v_2,\cdots,v_n)=1 for any orthonormal basis v_1,v_2,\cdots,v_n given an orientation for V.
Here is my question:
If \det(A)=-1, then f(u_1,u_2,\cdots,u_n)=-1, which makes f not unique