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sl(2)-subalgebras of sp(6), type C13

sp(6), type C13
Structure constants and notation.
Root subalgebras / root subsystems.
sl(2)-subalgebras.
Semisimple subalgebras.

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Number of sl(2) subalgebras: 7.
Let h be in the Cartan subalgebra. Let α1,...,αn be simple roots with respect to h. Then the h-characteristic, as defined by E. Dynkin, is the n-tuple (α1(h),...,αn(h)).

The actual realization of h. The coordinates of h are given with respect to the fixed original simple basis. Note that the h-characteristic is computed using a possibly different simple basis, more precisely, with respect to any h-positive simple basis.
A regular semisimple subalgebra might contain an sl(2) such that the sl(2) has no centralizer in the regular semisimple subalgebra, but the regular semisimple subalgebra might fail to be minimal containing. This happens when another minimal containing regular semisimple subalgebra of equal rank nests as a root subalgebra in the containing SA. See Dynkin, Semisimple Lie subalgebras of semisimple Lie algebras, remark before Theorem 10.4.
The sl(2) submodules of the ambient Lie algebra are parametrized by their highest weight with respect to the Cartan element h of sl(2). In turn, the highest weight is a positive integer multiple of the fundamental highest weight ψ. Vlψ is l+1-dimensional.


Type + realization linkh-CharacteristicRealization of hsl(2)-module decomposition of the ambient Lie algebra
ψ= the fundamental sl(2)-weight.
Centralizer dimensionType of semisimple part of centralizer, if knownThe square of the length of the weight dual to h.Dynkin index Minimal containing regular semisimple SAsContaining regular semisimple SAs in which the sl(2) has no centralizer
A351(2, 2, 2)(10, 16, 9)V10ψ+V6ψ+V2ψ
0 07035C^{1}_3; C^{1}_3;
A111(2, 0, 2)(6, 8, 5)V6ψ+V4ψ+3V2ψ
0 02211C^{1}_3; B^{1}_2+A^{1}_1; C^{1}_3; B^{1}_2+A^{1}_1;
A101(2, 1, 0)(6, 8, 4)V6ψ+2V3ψ+V2ψ+3V0
3 A112010B^{1}_2; B^{1}_2;
A81(0, 2, 0)(4, 8, 4)3V4ψ+V2ψ+3V0
3 not computed168A^{2}_2; A^{2}_2;
A31(0, 0, 2)(2, 4, 3)6V2ψ+3V0
3 not computed633A^{1}_1; A^{2}_1+A^{1}_1; 3A^{1}_1; A^{2}_1+A^{1}_1;
A21(0, 1, 0)(2, 4, 2)3V2ψ+4Vψ+4V0
4 A11422A^{1}_1; A^{2}_1; 2A^{1}_1; A^{2}_1;
A11(1, 0, 0)(2, 2, 1)V2ψ+4Vψ+10V0
10 B1221A^{1}_1; A^{1}_1;


Length longest root ambient algebra squared/4= 1/2

Given a root subsystem P, and a root subsubsystem P_0, in (10.2) of Semisimple subalgebras of semisimple Lie algebras, E. Dynkin defines a numerical constant e(P, P_0) (which we call Dynkin epsilon).
In Theorem 10.3, Dynkin proves that if an sl(2) is an S-subalgebra in the root subalgebra generated by P, such that it has characteristic 2 for all simple roots of P lying in P_0, then e(P, P_0)= 0. It turns out by direct computation that, in the current case of C^{1}_3, e(P,P_0)= 0 implies that an S-sl(2) subalgebra of the root subalgebra generated by P with characteristic with 2's in the simple roots of P_0 always exists. Note that Theorem 10.3 is stated in one direction only.

h-characteristic: (2, 2, 2)
Length of the weight dual to h: 70
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Containing regular semisimple subalgebra number 1: C^{1}_3
sl(2)-module decomposition of the ambient Lie algebra: V10ψ+V6ψ+V2ψ
Below is one possible realization of the sl(2) subalgebra.
h=9h3+16h2+10h1
e=9/5g3+4g2+5g1
The polynomial system that corresponds to finding the h, e, f triple:
2x1x410 2x2x516 x3x69 


h-characteristic: (2, 0, 2)
Length of the weight dual to h: 22
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Number of containing regular semisimple subalgebras: 2
Containing regular semisimple subalgebra number 1: C^{1}_3 Containing regular semisimple subalgebra number 2: B^{1}_2+A^{1}_1
sl(2)-module decomposition of the ambient Lie algebra: V6ψ+V4ψ+3V2ψ
Below is one possible realization of the sl(2) subalgebra.
h=5h3+8h2+6h1
e=2111/11022g7+1330/5511g5+201/167g468/5511g3+60/167g1
The polynomial system that corresponds to finding the h, e, f triple:
x4x10+x2x9x1x8 x5x9+x4x7x3x6 2x3x8+2x1x66 2x4x9+2x2x7+2x1x68 x5x10+2x4x9+x2x75 


h-characteristic: (2, 1, 0)
Length of the weight dual to h: 20
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Containing regular semisimple subalgebra number 1: B^{1}_2
sl(2)-module decomposition of the ambient Lie algebra: V6ψ+2V3ψ+V2ψ+3V0
Below is one possible realization of the sl(2) subalgebra.
h=4h3+8h2+6h1
e=4g7+3/2g1
The polynomial system that corresponds to finding the h, e, f triple:
2x2x46 2x1x38 x1x34 


h-characteristic: (0, 2, 0)
Length of the weight dual to h: 16
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Containing regular semisimple subalgebra number 1: A^{2}_2
sl(2)-module decomposition of the ambient Lie algebra: 3V4ψ+V2ψ+3V0
Below is one possible realization of the sl(2) subalgebra.
h=4h3+8h2+4h1
e=2g6+g2
The polynomial system that corresponds to finding the h, e, f triple:
2x1x34 2x2x4+2x1x38 2x1x34 


h-characteristic: (0, 0, 2)
Length of the weight dual to h: 6
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Number of containing regular semisimple subalgebras: 2
Containing regular semisimple subalgebra number 1: 3A^{1}_1 Containing regular semisimple subalgebra number 2: A^{2}_1+A^{1}_1
sl(2)-module decomposition of the ambient Lie algebra: 6V2ψ+3V0
Below is one possible realization of the sl(2) subalgebra.
h=3h3+4h2+2h1
e=g9+1/2g7+1/5g3
The polynomial system that corresponds to finding the h, e, f triple:
2x1x42 2x2x5+2x1x44 x3x6+x2x5+x1x43 


h-characteristic: (0, 1, 0)
Length of the weight dual to h: 4
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Number of containing regular semisimple subalgebras: 2
Containing regular semisimple subalgebra number 1: 2A^{1}_1 Containing regular semisimple subalgebra number 2: A^{2}_1
sl(2)-module decomposition of the ambient Lie algebra: 3V2ψ+4Vψ+4V0
Below is one possible realization of the sl(2) subalgebra.
h=2h3+4h2+2h1
e=g9+1/2g7
The polynomial system that corresponds to finding the h, e, f triple:
2x1x32 2x2x4+2x1x34 x2x4+x1x32 


h-characteristic: (1, 0, 0)
Length of the weight dual to h: 2
Simple basis ambient algebra w.r.t defining h: 3 vectors: (1, 0, 0), (0, 1, 0), (0, 0, 1)
Containing regular semisimple subalgebra number 1: A^{1}_1
sl(2)-module decomposition of the ambient Lie algebra: V2ψ+4Vψ+10V0
Below is one possible realization of the sl(2) subalgebra.
h=h3+2h2+2h1
e=g9
The polynomial system that corresponds to finding the h, e, f triple:
2x1x22 2x1x22 x1x21