- In condensed matter physics many particle states are labelled by particle momenta. Berry phase is associated with U(1) connection in this momentum space. Quantum metric means extension to Kähler metric involving both the U(1) connection and metric. It defines a distance between quantum states labelled by momenta at 2-D Fermi surface.
- Quantum metric in condensed matter sense is defined in momentum space, or rather, Fermi surface, rather than Hilbert space. Here I disagree with the claim of (see this). At Hilbert space level geometrization would replace the flat Kähler metric with a curved metric and replace global linear superposition with its local variant.
- What is essential for this interpretation, is that the momentum space (2-D Fermi sphere) is endowed with a Kähler geometry. Both momentum space and position space are geometrized.
- Space-times are 4-surfaces X4 in H=M4× CP2: this hypothesis geometrizes standard model interactions and solves the energy problem of general relativity. Holography = holomorphy hypothesis leads to an exactly solvable classical theory.
- M8 serves as the analog of 8-D momentum space for H=M4× CP2 and Y4 generalizes the notion of momentum space. One can define for the points of M8 Minkowskian inner product xy as a real part of their octonionic product.
- Space-time surfaces X4 in H=M4× CP2 have as M8 duals 4-surfaces Y4 in M8 related by M8-H duality. Y4 generalizes the notion of the Fermi sphere and can be regarded as the 4-D space of 4-momenta representing the dispersion relation (see this and this).
Associativity condition for the tangent space of Y4 defines the number theoretic dynamics of Y4 and local G2 transformations allow us to construct a general solutions Y4 from very simple basic solutions Y4(f) determined by the roots f(0)=0 of analytic functions f(o) with real coefficients, which can be restricted to an extension of rationals. Polynomials and rational functions f appear as important special cases and form hierarchies since basic arithmetic operations and functional composition produce new solutions.
- How to define the analog of quantum geometry?
- The values of functions f(o) can be regarded as octonions such that the imaginary part is proportional to the radial octonion unit and thus allows interpretation as an ordinary imaginary unit. For two tangent vectors of x, y of quaternionic Y4 the real part of xy defines Minkowskian inner product. The product xy is a quaternion and could be seen as a quaternionic analog of Kähler form. An analog of quaternion structure would be in question. Could this define the number theoretic version of quantum geometry?
- CP2 allows a quaternion structure but does not allow hyper-Kähler structure. Hyper-Kähler structure with 4 covariantly constant quaternionic units defined by metric and 3 covariantly constant Kähler forms is not possible for CP2. And define induced quaternionic structure in X4. Could one induce the metric and spinor curvature of X4 to Y4?
The quaternionic tangent spaces of Y4 are labelled by the points of CP2 and the corresponding CP2 point can be taken as a local coordinate of M8. The metric of Y4 could be induced from that of X4 by M8-H duality. In M4⊂ M8 degrees of freedom the inversion map M4→ M4⊂ H motivated by Uncertainty Principle defines the M8-H duality.
There are singularities at which the CP2 point associated with Y4 is not unique. In the case of CP2 type extremals the CP2 points form a 3-D surface X3 and X3 points correspond to single point y in Y4: Y4 has a coordinate singularity at y, y blows up to X3 in H.
See the article "Does M8-H duality reduce to local G2 symmetry?" or the chapter with the same title.
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.