Opened 4 years ago

Closed 4 years ago

#845 closed proposed feature (invalid)

mereotopology of solid physics

Reported by: anonymous Owned by: somebody
Priority: critical Milestone: 3-1-5 and higher
Component: dontKnow Version: 3-1-7
Keywords: mereotopology Cc: su.azadeh.2005@…


Let A be a ring, G a finite group acting on /i and y: G X G -) C&4), the units of/i, a map satisfying (1) y(g, 6) Hgg’, 6’) = g(W, 6’)) y(g, g’g”) for g, g’, d’ in G (2) y(e, g) = 1 = y(g, e) for g E G, e the identity element of G, (3) y(g, g’)kg’W) = &f(n)) y(g, g’> for g, g’ in G. Then the corresponding crossed product algebra /i * ?G, or /i x G for short, has an elements CgiEG A.-; ,gi li ~/i. Addition is componentwise, and multiplication is given by & = g(A)g and g, g2 = y(g, , g2) m. In this paper we assume that the values of y lie in the center Z(A) of/i. Hence the action of G on /i is given by a group homomorphism G-P Aut(/i), and (3) can be left out. In the special case that y is the trivial map we write /1G instead of/i * G, and the elements as C,c li gi. AG is then called a skew group ring. There is a lot of literature on skew group algebras and crossed product algebras, and on the relationship with the ring AC whose elements are those elements of A left fixed by G. Much work has been done on which properties of li are inherited by n * G or AC. Some of the work on the relationship between these rings has its roots in trying to develop a Galois theory for noncommutative rings. We refer to [3, 7, 13-15, 19, 21, 23-25, 27, 281 and their references.

Change History (1)

comment:1 Changed 4 years ago by hannes

Resolution: invalid
Status: newclosed
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