The real locus Λ σ A C * -action on CP 4 defined by

The real locus Λ σ A C * -action on CP 4 defined by

Source publication
Preprint
Full-text available
We provide a new family of indefinite Einstein-Weyl structures of signature (++-) on a 3-manifold, which are real analytic and space-like Zoll. They are obtained by using the minitwistor correspondence. The minitwistor spaces we use are Segre quartic surfaces of a particular type. They admit a $\mathbb C^*$-action and form a 1-dimensional moduli sp...

Contexts in source publication

Context 1
... these points are real for the real structure (X 2 , X 3 , X 4 ) −→ (X 2 , X 3 , X 4 ) induced from σ if and only if the real numbers a, b and c have the same sign; namely iff the inequalities γ > α > β or γ < α < β (2.6) hold. Under these inequalities, if we think of these four points as those on the circle Λ σ ≃ S 1 , the point λ i is adjacent to λ i+1 where the indices are counted modulo 4. (See Figure 1.) As above, each of the four fibers f −1 (λ i ) ⊂ S consists of two lines. ...
Context 2
... denote I 1 := (λ 1 , λ 2 ) and I 2 := (λ 3 , λ 4 ) for the open intervals in the circle Λ σ . (See Figure 1.) We denote S σ 1 and S σ 2 for the connected components of S σ , which are 2-spheres lying over the the closures of I 1 and I 2 in Λ σ respectively. ...
Context 3
... name J 2 (p), J 3 (p), J 4 (p) and J 5 (p) for these intervals, where we put the indices in such a way that J i (p) is adjacent to J i+1 (p) where J 6 (p) means J 1 (p), and that one of the two ends of J 2 (p) is the point H 1 (p). (See Figure 1, where the ends of all the intervals are concretely pinned down. They are determined in the sequel.) ...
Context 4
... p = q = p ′ , we understand the condition as that the branch of C u specified by p ′ is tangent to C at p. Under this kind of interpretation, even when {p, q} ∩ {p ′ , q ′′ } } = ∅, we can define C C p,q as in (4.14). In any case, o ∈ C C p,q . ...

Similar publications

Preprint
Full-text available
It has been unknown whether Hirota's discrete Korteweg-de Vries equation and the lattice sine-Gordon equation have the consistency around a cube (CAC) property. In this paper, we show that they have the CAC property. Moreover, we also show that they can be extended to systems on the 3-dimensional integer lattice.