Let g\mathfrak g and h\mathfrak h be over the same field.

The direct sum Lie algebra g⊕h\mathfrak g\oplus \mathfrak h is the direct sum as vector spaces equipped with the bracket

[(X1,Y1),(X2,Y2)]:=([X1,X2]g,  [Y1,Y2]h).[(X_1,Y_1),(X_2,Y_2)] := \bigl([X_1,X_2]_{\mathfrak g},\; [Y_1,Y_2]_{\mathfrak h}\bigr).

With this bracket, the inclusions g↪g⊕h\mathfrak g\hookrightarrow \mathfrak g\oplus\mathfrak h and h↪g⊕h\mathfrak h\hookrightarrow \mathfrak g\oplus\mathfrak h are , and g\mathfrak g and h\mathfrak h commute inside the sum.

Universal property

Giving a Lie algebra homomorphism g⊕h→k\mathfrak g\oplus\mathfrak h\to\mathfrak k is equivalent to giving homomorphisms g→k\mathfrak g\to\mathfrak k and h→k\mathfrak h\to\mathfrak k whose images commute.

Relation to Lie groups

If GG and HH are Lie groups, then the Lie algebra of the G×HG\times H is canonically

Lie(G×H)≅Lie(G)⊕Lie(H),\mathrm{Lie}(G\times H)\cong \mathrm{Lie}(G)\oplus \mathrm{Lie}(H),

as recorded in .

Context. Many decomposition results (e.g. ) are literally statements that a Lie algebra splits as a direct .