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How to define hypercomplex conjugation?

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It took a considerable time to realize that hyper complex conjugation u↔ w for the hypercomplex coordinates, which are real, might pose serious interpretational problems. Suppose that the roots of the generalized analytic maps f=(f1,f2)(u,w,ξ12): H→ C2 define the space-time surfaces.

What does one mean with the generalization of the complex conjugation when applied to the argument of f? Could it correspond a) to (u,w,ξ12)→ (u,w,ξ1,ξ2) so that there is no hypercomplex conjugation or b) to (v,w,ξ12)→ (u,w ,ξ1,ξ2) so that there is hypercomplex conjugation.

  1. For option a), the roots of f and f represent the same surface. For the roots of f the contribution of complex coordinates to guv and gvw is vanishing but the components guw.
  2. For option b), the roots of the conjugate f do not coincide with the roots of f unless symmetries (possibly non-local) exist. The condition u=v makes the two conditions equivalent. For the simplest option u=m0+m3, v= m0-m3 the condition u=v gives m3=0 and so that the intersection of the two roots is 3-D surface analogous to a particle at rest. Could this surface be identified as partonic orbit. If one accepts both roots, one has a situation similar to the option a) for both branches and branches intersect at the 3-D surface.

The basic idea is that partonic orbits are light-like with respect to 4-metric g4. Is it possible to realize this somehow for option b)? Could one assume that in the intersection of branches visualizable as intersection of two 1-D curves, the partial derivatives of complex H coordinates include both u and v derivatives so that the component guv of the induced metric receives an additional contribution from the complex coordinates. The partonic orbit would represent a violation of conformal symmetry in the sense that it would represent an intersection of analytic and anti-analytic region. In the case of ordinary violation of analyticity, the derivative of function f(z) is non-vanishing also with respect to z. The hypercomplex variant for the breaking of analyticity corresponds to the vanishing of the partial deritives of ξi with respect to both u and v.

  • The condition guv=0 does not follow automatically from the v=u condition which already selects a 3-surface as the intersection. This condition must however hold true if the partonic orbit defines the interface between the Minkowskian and Euclidean regions, which also has u-v doubling. guv=0 implies that 4-D tangent space is effectively 2-D at the partonic orbit. guv=0 condition at interface means cancellation of the M4 and CP2 contributions to the metric and guarantee the continuity of the Hermitian metric.
  • This could relate to the notion of exotic smooth structure (see this and this)? The intersecting u and v-lines indeed bring in mind the vertex for fermion-antifermion pair creation. See the article Holography= holomorphy vision and a more precise view of partonic orbits or the chapter Holography= holomorphy vision: analogues of elliptic curves and partonic orbits .
  • For a summary of earlier postings see Latest progress in TGD.

    For the lists of articles (most of them published in journals founded by Huping Hu) and books about TGD see this.


    Source: https://matpitka.blogspot.com/2025/06/how-to-define-hypercomplex-conjugation.html


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