Extensions Of Minimal Transformation Groups

Download Extensions Of Minimal Transformation Groups PDF/ePub or read online books in Mobi eBooks. Click Download or Read Online button to get Extensions Of Minimal Transformation Groups book now. This website allows unlimited access to, at the time of writing, more than 1.5 million titles, including hundreds of thousands of titles in various foreign languages.
Extensions of Minimal Transformation Groups

This edition is an almost exact translation of the original Russian text. A few improvements have been made in the present ation. The list of references has been enlarged to include some papers published more recently, and the latter are marked with an asterisk. THE AUTHOR vii LIST OF SYMBOLS M = M(X,T,rr. ) 1,3. 3 A(X,T) 2·7. 3 M(R) 2·9. 4 2 C [(Y ,T ,p) ,G,h] 3·16. 6 P = P(X,T,rr. ) 3,16. 12 1'3. 3 C9v [(Y ,T ,p) ,G,h] Px 2·8. 9 E = E(X,T,rr. ) 1,4. 7 Q = Q(X,T,rr. ) 1,3. 3 3,12. 8 Ey Q": = Q":(X ,T, rr. ) = Q#(X,T,rr. ) Ext[(Y,T,p),G,h] 3,16. 4 Ext9v[(Y,T,p),G,h] 3,16. 12 2·8. 31 Q":(R) = Q#(R) 3·13. 5 3,12. 12 Gy 3,15. 4 Sx(A) 2,8. 18 G(X,Y) SeA) 2·8. 22 2 3,16. 8 H [cY,T,rr. ),G,h] HE, (X,T,rr. ) = (X,T) 3'12. 12 1'1. 1 Y (X,T,rr. ,G,a) 4·21. 4 3'16. 1 Hef) HK(f) 4·21. 9 H(X,T) 2,7. 3 1- 3,19. 1 L = L(X,T,rr. ) 1,3. 3 viii I NTRODUCTI ON 1. It is well known that an autonomous system of ordinary dif ferential equations satisfying conditions that ensure uniqueness and extendibility of solutions determines a flow, i. e. a one parameter transformation group. G. D.
Extensions of Minimal Transformation Groups

This edition is an almost exact translation of the original Russian text. A few improvements have been made in the present- ation. The list of references has been enlarged to include some papers published more recently, and the latter are marked with an asterisk. THE AUTHOR vii LIST OF SYMBOLS M = M(X, T, rr. ) 1,3. 3 A(X, T) 2-7. 3 M(R) 2-9. 4 2 C [(Y, T, p), G, h] 3-16. 6 P = P(X, T, rr. ) 3,16. 12 1'3. 3 C9v [(Y, T, p), G, h] Px 2-8. 9 E = E(X, T, rr. ) 1,4. 7 Q = Q(X, T, rr. ) 1,3. 3 3,12. 8 Ey Q" = Q" (X, T, rr. ) = Q#(X, T, rr. ) Ext[(Y, T, p), G, h] 3,16. 4 Ext9v[(Y, T, p), G, h] 3,16. 12 2-8. 31 Q" (R) = Q#(R) 3-13. 5 3,12. 12 Gy 3,15. 4 Sx(A) 2,8. 18 G(X, Y) SeA) 2-8. 22 2 3,16. 8 H [cY, T, rr. ), G, h] HE, (X, T, rr. ) = (X, T) 3'12. 12 1'1. 1 Y (X, T, rr., G, a) 4-21. 4 3'16. 1 Hef) HK(f) 4-21. 9 H(X, T) 2,7. 3 1- 3,19. 1 L = L(X, T, rr. ) 1,3. 3 viii I NTRODUCTI ON 1. It is well known that an autonomous system of ordinary dif- ferential equations satisfying conditions that ensure uniqueness and extendibility of solutions determines a flow, i. e. a one- parameter transformation group. G. D.