Library / Lie Groups and Lie Algebras / Chapter III / § 5
Proposition 1
Tag 0AE1, permanent. Cite it as [Bourbaki, Tag 0AE1].
Lie Groups and Lie Algebras, chapter III, § 5. Formal calculations in Lie groups
(i)
x [ − 1 ] ≡ − x + B ( x , x ) m o d deg 3 x^{[-1]} \equiv -x + B(x, x) \mod \deg 3 x [ − 1 ] ≡ − x + B ( x , x ) mod deg 3 (ii)
x . y . x [ − 1 ] ≡ y + [ x , y ] m o d deg 3 x.y.x^{[-1]} \equiv y + [x, y] \mod \deg 3 x . y . x [ − 1 ] ≡ y + [ x , y ] mod deg 3 (iii)
y [ − 1 ] . x . y ≡ x + [ x , y ] m o d deg 3 y^{[-1]}.x.y \equiv x + [x, y] \mod \deg 3 y [ − 1 ] . x . y ≡ x + [ x , y ] mod deg 3 (iv)
x [ − 1 ] . y [ − 1 ] . x . y ≡ [ x , y ] m o d deg 3 x^{[-1]}.y^{[-1]}.x.y \equiv [x, y] \mod \deg 3 x [ − 1 ] . y [ − 1 ] . x . y ≡ [ x , y ] mod deg 3 (v)
x . y . x [ − 1 ] . y [ − 1 ] ≡ [ x , y ] m o d deg 3. x.y.x^{[-1]}.y^{[-1]} \equiv [x, y] \mod \deg 3. x . y . x [ − 1 ] . y [ − 1 ] ≡ [ x , y ] mod deg 3. (In (i),
x [ − 1 ] x^{[-1]} x [ − 1 ] of course represents the expansion of the function
x ↦ x [ − 1 ] x \mapsto x^{[-1]} x ↦ x [ − 1 ] as an integral series about the origin; the other formulae can be interpreted analogously.) Let
g 1 g_1 g 1 and
g 2 g_2 g 2 be the homogeneous components of
x [ − 1 ] x^{[-1]} x [ − 1 ] of degrees 1 and 2. Then
0 = x . x [ − 1 ] ≡ x + g 1 ( x ) + B ( x , g 1 ( x ) ) m o d deg 2 (by (6)) ≡ x + g 1 ( x ) m o d deg 2
0 = x.x^{[-1]} \\
\equiv x + g_1(x) + B(x, g_1(x)) \mod \deg 2 \quad \text{(by (6))} \\
\equiv x + g_1(x) \mod \deg 2
0 = x . x [ − 1 ] ≡ x + g 1 ( x ) + B ( x , g 1 ( x )) mod deg 2 (by (6)) ≡ x + g 1 ( x ) mod deg 2 and hence
g 1 ( x ) = − x g_1(x) = -x g 1 ( x ) = − x . Then
0 = x . x [ − 1 ] ≡ x + ( − x + g 2 ( x ) ) + B ( x , − x + g 2 ( x ) ) m o d deg 3 ≡ g 2 ( x ) − B ( x , x ) m o d deg 3
0 = x.x^{[-1]} \\
\equiv x + (-x + g_2(x)) + B(x, -x + g_2(x)) \mod \deg 3 \\
\equiv g_2(x) - B(x, x) \mod \deg 3
0 = x . x [ − 1 ] ≡ x + ( − x + g 2 ( x )) + B ( x , − x + g 2 ( x )) mod deg 3 ≡ g 2 ( x ) − B ( x , x ) mod deg 3
and hence g 2 ( x ) = B ( x , x ) g_2(x) = B(x, x) g 2 ( x ) = B ( x , x ) . This proves (i). Then, using (i),
x . y . x [ − 1 ] ≡ ( x + y + B ( x , y ) ) . ( − x + B ( x , x ) ) mod deg 3
x.y.x^{[-1]} \equiv (x + y + B(x, y)).(-x + B(x, x)) \quad \text{mod deg 3}
x . y . x [ − 1 ] ≡ ( x + y + B ( x , y )) . ( − x + B ( x , x )) mod deg 3 ≡ x + y + B ( x , y ) + ( − x + B ( x , x ) ) + B ( x + y , − x ) mod deg 3
\equiv x + y + B(x, y) + (-x + B(x, x)) + B(x + y, -x) \quad \text{mod deg 3}
≡ x + y + B ( x , y ) + ( − x + B ( x , x )) + B ( x + y , − x ) mod deg 3 ≡ y + B ( x , y ) − B ( y , x ) mod deg 3
\equiv y + B(x, y) - B(y, x) \quad \text{mod deg 3}
≡ y + B ( x , y ) − B ( y , x ) mod deg 3 ≡ y + [ x , y ] mod deg 3 (by (13))
\equiv y + [x, y] \quad \text{mod deg 3 (by (13))}
≡ y + [ x , y ] mod deg 3 (by (13)) whence (ii). The proof of (iii) is analogous. Combining (i) and (iii), we obtain
x [ − 1 ] , y [ − 1 ] . x . y ≡ ( − x + B ( x , x ) ) . ( x + [ x , y ] ) mod deg 3
x^{[-1]},y^{[-1]}.x.y \equiv (-x + B(x, x)).(x + [x, y]) \quad \text{mod deg 3}
x [ − 1 ] , y [ − 1 ] . x . y ≡ ( − x + B ( x , x )) . ( x + [ x , y ]) mod deg 3 ≡ − x + B ( x , x ) + x + [ x , y ] + B ( − x , x ) mod deg 3
\equiv -x + B(x, x) + x + [x, y] + B(-x, x) \quad \text{mod deg 3}
≡ − x + B ( x , x ) + x + [ x , y ] + B ( − x , x ) mod deg 3 ≡ [ x , y ] mod deg 3
\equiv [x, y] \quad \text{mod deg 3}
≡ [ x , y ] mod deg 3 whence (iv). The proof of (v) is analogous.
Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.
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Transcribed from the printed volume. Not translated.