generic derivation : delta:= mat((xi(1,1),xi(1,2),xi(1,3),xi(1,4),0,0),(xi(2,1),xi(2,2),xi(1,4),xi(2,4),0,0), (xi(3,1),xi(3,2),xi(3,3), - xi(2,1),0,0),(xi(3,2),xi(4,2), - xi(1,2),xi(3,3) - xi(2,2) + xi(1,1),0,0),(xi(5,1),xi(5,2),xi(5,3),xi(5,4),xi(3,3) + xi(1,1),xi(5,6 )),(xi(6,1),xi(6,2),xi(6,3),xi(6,4),0,xi(6,6)))$ [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] adx1 := [ ] [0 0 0 0 0 0] [ ] [0 0 1 0 0 0] [ ] [0 0 0 0 0 0] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] adx2 := [ ] [0 0 0 0 0 0] [ ] [0 0 0 1 0 0] [ ] [0 0 0 0 0 0] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] adx3 := [ ] [0 0 0 0 0 0] [ ] [-1 0 0 0 0 0] [ ] [0 0 0 0 0 0] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] adx4 := [ ] [0 0 0 0 0 0] [ ] [0 -1 0 0 0 0] [ ] [0 0 0 0 0 0] The generic nilpotent derivation : the eigenvalues are 0 xi(3,3):= - xi(1,1) xi(6,6):=0 And the matrix A:= [xi(1,1) xi(1,2) xi(1,3) xi(1,4) ] [ ] [xi(2,1) xi(2,2) xi(1,4) xi(2,4) ] [ ] [xi(3,1) xi(3,2) - xi(1,1) - xi(2,1)] [ ] [xi(3,2) xi(4,2) - xi(1,2) - xi(2,2)] is nilpotent. [xi(1,1) xi(1,2) xi(1,3) xi(1,4) ] [ ] [xi(2,1) xi(2,2) xi(1,4) xi(2,4) ] m := [ ] [xi(3,1) xi(3,2) - xi(1,1) - xi(2,1)] [ ] [xi(3,2) xi(4,2) - xi(1,2) - xi(2,2)] we may suppose that A is an element of sp(4,C)+, that is: xi(1,1):=0 xi(2,1):=0 xi(2,2):=0 xi(3,1):=0 xi(3,2):=0 xi(4,2):=0 M**1:= [0 xi(1,2) xi(1,3) xi(1,4)] [ ] [0 0 xi(1,4) xi(2,4)] [ ] [0 0 0 0 ] [ ] [0 0 - xi(1,2) 0 ] M**2:= [0 0 0 xi(2,4)*xi(1,2)] [ ] [0 0 - xi(2,4)*xi(1,2) 0 ] [ ] [0 0 0 0 ] [ ] [0 0 0 0 ] M**3:= [ 2 ] [0 0 - xi(2,4)*xi(1,2) 0] [ ] [0 0 0 0] [ ] [0 0 0 0] [ ] [0 0 0 0] M**4:= [0 0 0 0] [ ] [0 0 0 0] [ ] [0 0 0 0] [ ] [0 0 0 0] Trace(M**1)/2:=0$ Trace(M**2)/2:=0$ Trace(M**3)/2:=0$ Trace(M**4)/2:=0$ ************************************************************************$ *******Suppose xi(1,2) neq 0.$ ************************************************************************$ By subtracting adjoints one then may suppose:$ xi(5,1):=0,xi(5,2):=0,xi(5,3):=0,xi(5,4):=0$ delta:= [ 0 xi(1,2) xi(1,3) xi(1,4) 0 0 ] [ ] [ 0 0 xi(1,4) xi(2,4) 0 0 ] [ ] [ 0 0 0 0 0 0 ] [ ] [ 0 0 - xi(1,2) 0 0 0 ] [ ] [ 0 0 0 0 0 xi(5,6)] [ ] [xi(6,1) xi(6,2) xi(6,3) xi(6,4) 0 0 ] We denote this delta by the shortform$ shortformdelta:={xi(1,2), xi(1,3), xi(1,4), ss, xi(2,4), ss, xi(5,6), ss, xi(6,1), xi(6,2), xi(6,3), xi(6,4)}$ paramindexeslist:={{1,2},{1,3},{1,4},{2,4},{5,6},{6,1},{6,2},{6,3},{6,4}}$ a:=0$ b:=0$ delta:= [0 0 1 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 1] [ ] [0 0 0 0 0 0] shortformdelta:={0,1,0,ss,0,ss,1,ss,0,0,0,0}$ on resout l'equation {{0,1},1} qui est maintenant AA:=d(3,1)$ Unknown: d(3,1) Unknown: d(3,1) bonne inconnue W:=d(3,1)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,1},5} qui est maintenant AA:=d(6,1) - d(3,0)$ Unknowns: {d(6,1),d(3,0)} Unknowns: {d(6,1),d(3,0)} bonne inconnue W:=d(6,1)$ sa valeur doit etre WW:=d(3,0)$ on resout l'equation {{0,2},1} qui est maintenant AA:=d(3,2)$ Unknown: d(3,2) Unknown: d(3,2) bonne inconnue W:=d(3,2)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,2},5} qui est maintenant AA:=d(6,2) - d(4,0)$ Unknowns: {d(6,2),d(4,0)} Unknowns: {d(6,2),d(4,0)} bonne inconnue W:=d(6,2)$ sa valeur doit etre WW:=d(4,0)$ on resout l'equation {{0,3},0} qui est maintenant AA:= - d(0,1)$ Unknown: d(0,1) Unknown: d(0,1) bonne inconnue W:=d(0,1)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,3},1} qui est maintenant AA:=d(3,3) - d(1,1) + d(0,0)$ Unknowns: {d(3,3),d(1,1),d(0,0)} Unknowns: {d(3,3),d(1,1),d(0,0)} bonne inconnue W:=d(3,3)$ sa valeur doit etre WW:=d(1,1) - d(0,0)$ on resout l'equation {{0,3},2} qui est maintenant AA:= - d(2,1)$ Unknown: d(2,1) Unknown: d(2,1) bonne inconnue W:=d(2,1)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,3},4} qui est maintenant AA:= - d(4,1)$ Unknown: d(4,1) Unknown: d(4,1) bonne inconnue W:=d(4,1)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,3},5} qui est maintenant AA:=d(6,3) - d(5,1) + d(1,0)$ Unknowns: {d(6,3),d(5,1),d(1,0)} Unknowns: {d(6,3),d(5,1),d(1,0)} bonne inconnue W:=d(6,3)$ sa valeur doit etre WW:=d(5,1) - d(1,0)$ on resout l'equation {{0,3},6} qui est maintenant AA:= - d(3,0)$ Unknown: d(3,0) Unknown: d(3,0) bonne inconnue W:=d(3,0)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,4},1} qui est maintenant AA:=d(3,4)$ Unknown: d(3,4) Unknown: d(3,4) bonne inconnue W:=d(3,4)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,4},5} qui est maintenant AA:=d(6,4) + d(2,0)$ Unknowns: {d(6,4),d(2,0)} Unknowns: {d(6,4),d(2,0)} bonne inconnue W:=d(6,4)$ sa valeur doit etre WW:= - d(2,0)$ on resout l'equation {{0,5},1} qui est maintenant AA:=d(3,5)$ Unknown: d(3,5) Unknown: d(3,5) bonne inconnue W:=d(3,5)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,5},5} qui est maintenant AA:=d(6,5)$ Unknown: d(6,5) Unknown: d(6,5) bonne inconnue W:=d(6,5)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,6},0} qui est maintenant AA:= - d(0,5)$ Unknown: d(0,5) Unknown: d(0,5) bonne inconnue W:=d(0,5)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,6},1} qui est maintenant AA:=d(3,6) - d(1,5)$ Unknowns: {d(3,6),d(1,5)} Unknowns: {d(3,6),d(1,5)} bonne inconnue W:=d(3,6)$ sa valeur doit etre WW:=d(1,5)$ on resout l'equation {{0,6},2} qui est maintenant AA:= - d(2,5)$ Unknown: d(2,5) Unknown: d(2,5) bonne inconnue W:=d(2,5)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,6},4} qui est maintenant AA:= - d(4,5)$ Unknown: d(4,5) Unknown: d(4,5) bonne inconnue W:=d(4,5)$ sa valeur doit etre WW:=0$ on resout l'equation {{0,6},5} qui est maintenant AA:=d(6,6) - d(5,5) + d(0,0)$ Unknowns: {d(6,6),d(5,5),d(0,0)} Unknowns: {d(6,6),d(5,5),d(0,0)} bonne inconnue W:=d(6,6)$ sa valeur doit etre WW:=d(5,5) - d(0,0)$ on resout l'equation {{1,3},1} qui est maintenant AA:= - d(1,5)$ Unknown: d(1,5) Unknown: d(1,5) bonne inconnue W:=d(1,5)$ sa valeur doit etre WW:=0$ on resout l'equation {{1,3},5} qui est maintenant AA:= - d(5,5) + 2*d(1,1) - d( 0,0)$ Unknowns: {d(5,5),d(1,1),d(0,0)} Unknowns: {d(5,5),d(1,1),d(0,0)} bonne inconnue W:=d(5,5)$ sa valeur doit etre WW:=2*d(1,1) - d(0,0)$ on resout l'equation {{2,3},1} qui est maintenant AA:=d(0,2)$ Unknown: d(0,2) Unknown: d(0,2) bonne inconnue W:=d(0,2)$ sa valeur doit etre WW:=0$ on resout l'equation {{2,3},5} qui est maintenant AA:=d(4,3) + d(1,2)$ Unknowns: {d(4,3),d(1,2)} Unknowns: {d(4,3),d(1,2)} bonne inconnue W:=d(4,3)$ sa valeur doit etre WW:= - d(1,2)$ on resout l'equation {{2,4},5} qui est maintenant AA:=d(4,4) + d(2,2) - 2*d(1,1 ) + d(0,0)$ Unknowns: {d(4,4),d(2,2),d(1,1),d(0,0)} Unknowns: {d(4,4),d(2,2),d(1,1),d(0,0)} bonne inconnue W:=d(4,4)$ sa valeur doit etre WW:= - d(2,2) + 2*d(1,1) - d(0,0)$ on resout l'equation {{2,6},5} qui est maintenant AA:=d(4,6)$ Unknown: d(4,6) Unknown: d(4,6) bonne inconnue W:=d(4,6)$ sa valeur doit etre WW:=0$ on resout l'equation {{3,4},1} qui est maintenant AA:= - d(0,4)$ Unknown: d(0,4) Unknown: d(0,4) bonne inconnue W:=d(0,4)$ sa valeur doit etre WW:=0$ on resout l'equation {{3,4},5} qui est maintenant AA:=d(2,3) - d(1,4)$ Unknowns: {d(2,3),d(1,4)} Unknowns: {d(2,3),d(1,4)} bonne inconnue W:=d(2,3)$ sa valeur doit etre WW:=d(1,4)$ on resout l'equation {{3,6},1} qui est maintenant AA:= - d(0,6)$ Unknown: d(0,6) Unknown: d(0,6) bonne inconnue W:=d(0,6)$ sa valeur doit etre WW:=0$ on resout l'equation {{3,6},5} qui est maintenant AA:= - d(1,6) + d(0,3)$ Unknowns: {d(1,6),d(0,3)} Unknowns: {d(1,6),d(0,3)} bonne inconnue W:=d(1,6)$ sa valeur doit etre WW:=d(0,3)$ on resout l'equation {{4,6},5} qui est maintenant AA:= - d(2,6)$ Unknown: d(2,6) Unknown: d(2,6) bonne inconnue W:=d(2,6)$ sa valeur doit etre WW:=0$ Derivation equations to cancel (Reduce output) : \\{{{{0,1},1},0}, {{{0,1},5},0}, {{{0,2},1},0}, {{{0,2},5},0}, {{{0,3},0},0}, {{{0,3},1},0}, {{{0,3},2},0}, {{{0,3},3},0}, {{{0,3},4},0}, {{{0,3},5},0}, {{{0,3},6},0}, {{{0,4},1},0}, {{{0,4},5},0}, {{{0,5},1},0}, {{{0,5},5},0}, {{{0,6},0},0}, {{{0,6},1},0}, {{{0,6},2},0}, {{{0,6},3},0}, {{{0,6},4},0}, {{{0,6},5},0}, {{{0,6},6},0}, {{{1,2},5},0}, {{{1,3},0},0}, {{{1,3},1},0}, {{{1,3},2},0}, {{{1,3},3},0}, {{{1,3},4},0}, {{{1,3},5},0}, {{{1,3},6},0}, {{{1,4},5},0}, {{{1,5},5},0}, {{{1,6},5},0}, {{{2,3},1},0}, {{{2,3},5},0}, {{{2,4},0},0}, {{{2,4},1},0}, {{{2,4},2},0}, {{{2,4},3},0}, {{{2,4},4},0}, {{{2,4},5},0}, {{{2,4},6},0}, {{{2,5},5},0}, {{{2,6},5},0}, {{{3,4},1},0}, {{{3,4},5},0}, {{{3,5},1},0}, {{{3,5},5},0}, {{{3,6},1},0}, {{{3,6},5},0}, {{{4,5},5},0}, {{{4,6},5},0}, {{{5,6},5},0}}$ Il n'y a pas de phase 2$ derivation generique de gtildedelta:$ MATD:= mat((d(0,0),0,0,d(0,3),0,0,0),(d(1,0),d(1,1),d(1,2),d(1,3),d(1,4),0,d(0,3)),(d(2 ,0),0,d(2,2),d(1,4),d(2,4),0,0),(0,0,0,d(1,1) - d(0,0),0,0,0),(d(4,0),0,d(4,2), - d(1,2), - d(2,2) + 2*d(1,1) - d(0,0),0,0),(d(5,0),d(5,1),d(5,2),d(5,3),d(5,4), 2*d(1,1) - d(0,0),d(5,6)),(d(6,0),0,d(4,0),d(5,1) - d(1,0), - d(2,0),0,2*(d(1,1) - d(0,0))))$ pour delta:= [0 0 1 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 0] [ ] [0 0 0 0 0 1] [ ] [0 0 0 0 0 0] pour shortformdelta:={0,1,0,ss,0,ss,1,ss,0,0,0,0} Unknowns: {d(6,0), d(5,6), d(5,4), d(5,3), d(5,2), d(5,1), d(5,0), d(4,2), d(4,0), d(2,4), d(2,2), d(2,0), d(1,4), d(1,3), d(1,2), d(1,1), d(1,0), d(0,3), d(0,0)} Unknowns: {d(6,0), d(5,6), d(5,4), d(5,3), d(5,2), d(5,1), d(5,0), d(4,2), d(4,0), d(2,4), d(2,2), d(2,0), d(1,4), d(1,3), d(1,2), d(1,1), d(1,0), d(0,3), d(0,0)} listeparametresMATD{d(6,0), d(5,6), d(5,4), d(5,3), d(5,2), d(5,1), d(5,0), d(4,2), d(4,0), d(2,4), d(2,2), d(2,0), d(1,4), d(1,3), d(1,2), d(1,1), d(1,0), d(0,3), d(0,0)}$ dim Der(gtildedelta):=19$ t1:=D(0,0):= [1 0 0 0 0 0 0 ] [ ] [0 0 0 0 0 0 0 ] [ ] [0 0 0 0 0 0 0 ] [ ] [0 0 0 -1 0 0 0 ] [ ] [0 0 0 0 -1 0 0 ] [ ] [0 0 0 0 0 -1 0 ] [ ] [0 0 0 0 0 0 -2] Unknowns: {d(5,4),d(5,3),d(2,2),d(1,2),d(1,1),d(0,0)} Unknowns: {d(5,4),d(5,3),d(2,2),d(1,2),d(1,1),d(0,0)} commutant de t1 dans der(gtildedelta): mat((d(0,0),0,0,0,0,0,0), (0,d(1,1),d(1,2),0,0,0,0), (0,0,d(2,2),0,0,0,0), (0,0,0,d(1,1) - d(0,0),0,0,0), (0,0,0, - d(1,2), - d(2,2) + 2*d(1,1) - d(0,0),0,0), (0,0,0,d(5,3),d(5,4),2*d(1,1) - d(0,0),0), (0,0,0,0,0,0,2*(d(1,1) - d(0,0)))) Unknowns: {d(5,4),d(5,3),d(2,2),d(1,2),d(1,1),d(0,0)} Unknowns: {d(5,4),d(5,3),d(2,2),d(1,2),d(1,1),d(0,0)} t2:=D(1,1):= [0 0 0 0 0 0 0] [ ] [0 1 0 0 0 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 0 1 0 0 0] [ ] [0 0 0 0 2 0 0] [ ] [0 0 0 0 0 2 0] [ ] [0 0 0 0 0 0 2] Unknowns: {d(5,4),d(2,2),d(1,1),d(0,0)} Unknowns: {d(5,4),d(2,2),d(1,1),d(0,0)} commutant simultane de t1,t2 dans der(gtildedelta):$ mat((d(0,0),0,0,0,0,0,0),(0,d(1,1),0,0,0,0,0),(0,0,d(2,2),0,0,0,0),(0,0,0,d(1,1) - d(0,0),0,0,0),(0,0,0,0, - d(2,2) + 2*d(1,1) - d(0,0),0,0),(0,0,0,0,d(5,4),2*d (1,1) - d(0,0),0),(0,0,0,0,0,0,2*(d(1,1) - d(0,0))))$ Unknowns: {d(5,4),d(2,2),d(1,1),d(0,0)} Unknowns: {d(5,4),d(2,2),d(1,1),d(0,0)} t3:=D(2,2):= [0 0 0 0 0 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 1 0 0 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 0 0 -1 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 0 0 0 0 0] Unknowns: {d(2,2),d(1,1),d(0,0)} Unknowns: {d(2,2),d(1,1),d(0,0)} commutant simultane de t1,t2,t3 dans der(gtildedelta): mat((d(0,0),0,0,0,0,0,0), (0,d(1,1),0,0,0,0,0), (0,0,d(2,2),0,0,0,0), (0,0,0,d(1,1) - d(0,0),0,0,0), (0,0,0,0, - d(2,2) + 2*d(1,1) - d(0,0),0,0), (0,0,0,0,0,2*d(1,1) - d(0,0),0), (0,0,0,0,0,0,2*(d(1,1) - d(0,0)))) rank 3 with maximal torus t1,t2,t3 3 matrice de passage de la base X(0)=delta, X(1),..., X(6) a une base diagonali\ sant le tore maximal: on peut prendre P:= [1 0 0 0 0 0 0] [ ] [0 1 0 0 0 0 0] [ ] [0 0 1 0 0 0 0] [ ] [0 0 0 1 0 0 0] [ ] [0 0 0 0 1 0 0] [ ] [0 0 0 0 0 1 0] [ ] [0 0 0 0 0 0 1] P**(-1)*t1*P:= [1 0 0 0 0 0 0 ] [ ] [0 0 0 0 0 0 0 ] [ ] [0 0 0 0 0 0 0 ] [ ] [0 0 0 -1 0 0 0 ] [ ] [0 0 0 0 -1 0 0 ] [ ] [0 0 0 0 0 -1 0 ] [ ] [0 0 0 0 0 0 -2] P**(-1)*t2*P:= [0 0 0 0 0 0 0] [ ] [0 1 0 0 0 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 0 1 0 0 0] [ ] [0 0 0 0 2 0 0] [ ] [0 0 0 0 0 2 0] [ ] [0 0 0 0 0 0 2] P**(-1)*t3*P:= [0 0 0 0 0 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 1 0 0 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 0 0 -1 0 0] [ ] [0 0 0 0 0 0 0] [ ] [0 0 0 0 0 0 0] matrice des derivations dans cette base diagonalisante Y(1),...,Y(7): P**(-1)*MATD*P:= mat((d(0,0),0,0,d(0,3),0,0,0),(d(1,0),d(1,1),d(1,2),d(1,3),d(1,4),0,d(0,3)),(d(2 ,0),0,d(2,2),d(1,4),d(2,4),0,0),(0,0,0,d(1,1) - d(0,0),0,0,0),(d(4,0),0,d(4,2), - d(1,2), - d(2,2) + 2*d(1,1) - d(0,0),0,0),(d(5,0),d(5,1),d(5,2),d(5,3),d(5,4), 2*d(1,1) - d(0,0),d(5,6)),(d(6,0),0,d(4,0),d(5,1) - d(1,0), - d(2,0),0,2*(d(1,1) - d(0,0))))$ PP:= [1 0 0 0 0 0 0] [ ] [0 1 0 0 0 0 0] [ ] [0 0 1 0 0 0 0] [ ] [0 0 0 1 0 0 0] [ ] [0 0 0 0 1 0 0] [ ] [0 0 0 0 0 1 0] [ ] [0 0 0 0 0 0 1] avec PP:=P*Q:= [1 0 0 0 0 0 0] [ ] [0 1 0 0 0 0 0] [ ] [0 0 1 0 0 0 0] [ ] [0 0 0 1 0 0 0] [ ] [0 0 0 0 1 0 0] [ ] [0 0 0 0 0 1 0] [ ] [0 0 0 0 0 0 1] MATDDIAGONALISE:= mat((d(0,0),0,0,d(0,3),0,0,0), (d(1,0),d(1,1),d(1,2),d(1,3),d(1,4),0,d(0,3)), (d(2,0),0,d(2,2),d(1,4),d(2,4),0,0), (0,0,0,d(1,1) - d(0,0),0,0,0), (d(4,0),0,d(4,2), - d(1,2), - d(2,2) + 2*d(1,1) - d(0,0),0,0), (d(5,0),d(5,1),d(5,2),d(5,3),d(5,4),2*d(1,1) - d(0,0),d(5,6)), (d(6,0),0,d(4,0),d(5,1) - d(1,0), - d(2,0),0,2*(d(1,1) - d(0,0)))) on voit apparaitre les poids sur la diagonale r(1) := d(0,0) r(2) := d(1,1) r(3) := d(2,2) r(4) := d(1,1) - d(0,0) r(5) := - d(2,2) + 2*d(1,1) - d(0,0) r(6) := 2*d(1,1) - d(0,0) r(7) := 2*(d(1,1) - d(0,0)) r(1) := gamma2 r(2) := gamma1 + gamma2 r(3) := gamma2 - gamma3 + 2*gamma1 r(4) := gamma1 r(5) := gamma3 r(6) := 2*gamma1 + gamma2 r(7) := 2*gamma1 Le systeme de poids est le systeme 3.18 calcul de relations de commutation de la base diaY(j) diagonalisant le tore listcommutateursdesx := {{{0,1},0}, {{0,2},0}, {{0,3},x(1)}, {{0,4},0}, {{0,5},0}, {{0,6},x(5)}, {{1,2},0}, {{1,3},x(5)}, {{1,4},0}, {{1,5},0}, {{1,6},0}, {{2,3},0}, {{2,4},x(5)}, {{2,5},0}, {{2,6},0}, {{3,4},0}, {{3,5},0}, {{3,6},0}, {{4,5},0}, {{4,6},0}, {{5,6},0}} diaY(1):=x(0) diaY(2):=x(1) diaY(3):=x(2) diaY(4):=x(3) diaY(5):=x(4) diaY(6):=x(5) diaY(7):=x(6) liste des commutateurs des diaY(i) :$ listcommutateurdesdiaY:={{{1,2},0}, {{1,3},0}, {{1,4},diay(2)}, {{1,5},0}, {{1,6},0}, {{1,7},diay(6)}, {{2,3},0}, {{2,4},diay(6)}, {{2,5},0}, {{2,6},0}, {{2,7},0}, {{3,4},0}, {{3,5},diay(6)}, {{3,6},0}, {{3,7},0}, {{4,5},0}, {{4,6},0}, {{4,7},0}, {{5,6},0}, {{5,7},0}, {{6,7},0}}$ Now we make explicit the isomorphism with an algebra of the book:$ Namely g_{7,3.18}$ i.e. we go from the basis diaY(i) to the new basis ZZ(i) defined by the matrix:$ on pose :$ avec comme matrice de changement de base :$ mat((0,1,0,0,0,0,0),(0,0,0,0,0,-1,0),(0,0,0,-1,0,0,0),(1,0,0,0,0,0,0),(0,0,1,0,0 ,0,0),(0,0,0,0,0,0,1),(0,0,0,0,1,0,0))$ det(isom):= 1$ ZZ(1):=diay(4)$ ZZ(2):=diay(1)$ ZZ(3):=diay(5)$ ZZ(4):= - diay(3)$ ZZ(5):=diay(7)$ ZZ(6):= - diay(2)$ ZZ(7):=diay(6)$ listcommutateursdesZZ:=$ {{1,2},zz(6)}$ {{1,3},0}$ {{1,4},0}$ {{1,5},0}$ {{1,6},zz(7)}$ {{1,7},0}$ {{2,3},0}$ {{2,4},0}$ {{2,5},zz(7)}$ {{2,6},0}$ {{2,7},0}$ {{3,4},zz(7)}$ {{3,5},0}$ {{3,6},0}$ {{3,7},0}$ {{4,5},0}$ {{4,6},0}$ {{4,7},0}$ {{5,6},0}$ {{5,7},0}$ {{6,7},0}$ We get the commutation relations of$ g_{7,3.18}$ Et cela pour a:=0, b:=0.$ shortformdelta:={0,1,0,ss,0,ss,1,ss,0,0,0,0}$ delta:= mat((0,0,1,0,0,0),(0,0,0,0,0,0),(0,0,0,0,0,0),(0,0,0,0,0,0),(0,0,0,0,0,1),(0,0,0 ,0,0,0))$ The isomorphism from g_{7,3.18} to gtildedelta$ was constructed in 2 steps and is given by$ the product matrix P*isom:= mat((0,1,0,0,0,0,0),(0,0,0,0,0,-1,0),(0,0,0,-1,0,0,0),(1,0,0,0,0,0,0),(0,0,1,0,0 ,0,0),(0,0,0,0,0,0,1),(0,0,0,0,1,0,0))$ which we record here under the name PSI$