2011
DOI: 10.1007/s00209-011-0849-z
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Harmonic maps of finite uniton number into G 2

Abstract: We establish explicit formulae for canonical factorizations of extended solutions corresponding to harmonic maps of finite uniton number into the exceptional Lie group G 2 in terms of the Grassmannian model for the group of based algebraic loops in G 2 . A description of the "Frenet frame data" for such harmonic maps is given. In particular, we show that harmonic spheres into G 2 correspond to solutions of certain algebraic systems of quadratic and cubic equations.

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Cited by 7 publications
(17 citation statements)
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“…3. Recently there have been several publications concerning harmonic maps into compact Lie groups and compact symmetric spaces which have used methods which are different from ours, see [18], [9], [25] and reference therein. Most of their work basically follows the techniques developed by Uhlenbeck [26] and Segal [24].…”
Section: Proof Of Theorem 14mentioning
confidence: 99%
“…3. Recently there have been several publications concerning harmonic maps into compact Lie groups and compact symmetric spaces which have used methods which are different from ours, see [18], [9], [25] and reference therein. Most of their work basically follows the techniques developed by Uhlenbeck [26] and Segal [24].…”
Section: Proof Of Theorem 14mentioning
confidence: 99%
“…We have σ ̺,1 (X 1,2 ) = −X 3,4 and σ ̺,1 (X 1,3 ) = X 2,4 . Hence we can write C = C 0 + C 1 λ, with C 0 = a(X 1,2 − X 3,4 ) + b(X 1,3 + X 2,4 ), C 1 = cX 1,4 for some meromorphic functions a, b, c on S 2 . The harmonicity equations impose that ab ′ − ba ′ = 0, which means that b = αa for some constant α ∈ C. Hence given arbitrary meromorphic functions a, c on S 2 and a complex constant α,…”
Section: 31mentioning
confidence: 99%
“…The simple connected Lie group Spin (7), seen as a subgroup of SO(8) via spinor representation, is given, up to conjugation, by [15] for details). Hence, the Grassmannian model of ΩSpin (7) with respect to the spinor representation is given by the following proposition, whose proof we omit since it is completely similar to that of Proposition 3.2 in [9]. Fix on ∧ • U, where U = span{e 1 , e 2 , e 3 }, the vector basis…”
Section: Canonical Elements Of Classical Lie Algebrasmentioning
confidence: 99%