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20 Nov 2015: Every linear transformation is rotation dilation rotation via SVD. Trick is to double size of space. ... Blades] [Blades]. AB=simplify([bladeprod(a,b) | a <- A, b <- B]). Form every combination of product.

20 Nov 2015: Every linear transformation is rotation dilation rotation via SVD. Trick is to double size of space. ... Blades]. [Blades]. AB=simplify([bladeprod(a,b) | a <- A, b <- B]). Form every combination of product from the two lists.

3 Nov 2016: L7 S19. [Blades] [Blades]. AB=simplify([bladeprod(a,b) | a <- A, b <- B]). ... Form every combination of product from the two lists. Sort by grade and then integer order.

3 Nov 2016: L7 S19. [Blades]. [Blades]. AB=simplify([bladeprod(a,b) | a <- A, b <- B]). ... Form every combination of product from the two lists. Sort by grade and then integer order.

18 Feb 2015: We use the symmetric tensor hab to define aspatial covariant derivative (3)a which acting on a tensor T b.cd.e returns a tensorwhich is orthogonal to ua on every ... T (b)ab = ρ(b)uaub 2(ρ(b) p(b))u(av(b)b) p(b)hab, (2.17). which shows that the baryon

5 Feb 2015: Thus, every determinant of rank r can berepresented by. A B = 〈AB 〉0 , (3.9)where A = 〈A〉r is in Λrn and B = 〈B 〉s is in Λsn. ... It can be shown that every rotor can be expressed in the exponential form.