_{K}. The field equation is a geometric generalization of d'Alembert (Laplace) equation in Minkowskian (Eucidian) regions of space-time surface coupled with induced Kähler form analogous to Maxwell field. Generalization of equations of motion for particle by replacing it with 3-D surface is in question and the orbit of particle defines a region of space-time surface.

- Zero energy ontology (ZEO) suggests that the external particles arriving to the boundaries of given causal diamond (CD) are like free massless particles and correspond to minimal surfaces as a generalization of light-like geodesic. This dynamic reduces to mere algebraic conditions and there is no dependence on the coupling parameters of S. In contrast to this, in the interaction regions inside CDs there could be a coupling between Vol and S
_{K}due to the non-vanishing divergences of energy momentum currents associated with the two terms in action cancelling each other.

- Similar algebraic picture emerges from M
^{8}-H duality at the level of M^{8}and from what is known about preferred extremals of S assumed to satisfy infinite number of super-symplectic gauge conditions at the 3-surfaces defining the ends of space-time surface at the opposite boundaries of CD.

- At M
^{8}side of M^{8}-H duality associativity is realized as quaternionicity of either tangent or normal space of the space-time surface. The condition that there is 2-D integral distribution of sub-spaces of tangent spaces defining a distribution of complex planes as subspaces of octonionic tangent space implies the map of the space-time surface in M^{8}to that of H. Given point m_{8}of M^{8}is mapped to a point of M^{4}× CP_{2}as a pair of points (m_{4},s) formed by M^{4}⊂ M^{8}projection m_{4}of m_{8}point and by CP_{2}point s parameterizing the tangent space or the normal space of X^{4}⊂ M^{8}.

- If associativity or even the condition about the existence of the integrable distribution of 2-planes fails, the map to M
^{4}× CP_{2}is lost. One could cope with the situation since the gauge conditions at the boundaries of CD would allow to construct preferred extremal connecting the 3-surfaces at the boundaries of CD if this kind of surface exists at all. One can however wonder whether giving up the map M^{8}→ H is necessary.

- Number theoretic dynamics in M
^{8}involves no action principle and no coupling constants, just the associativity and the integrable distribution of complex planes M^{2}(x) of complexified octonions. This suggests that also the dynamics at the level of H involves coupling constants only via boundary conditions. This is the case for the minimal surface solutions suggesting that M^{8}-H duality maps the surfaces satisfying the above mentioned conditions to minimal surfaces. The universal dynamics conforms also with quantum criticality.

- One can argue that the dependence of field equations on coupling parameters in interactions leading to a perturbative series in coupling parameters in the interior of the space-time surface spoils the extremely beautiful purely algebraic picture about the construction of solutions of field equations using conformal invariance assignable to quantum criticality. Classical perturbation series is also in conflict with the vision that the TGD counterparts twistorial Grassmannian amplitudes do not involve any loop contributions coming as powers of coupling constant parameters.

^{8}-H duality, number theoretic vision, quantum criticality, twistor lift of TGD reducing dynamics to the condition about the existence of induced twistor structure, and the proposal for the construction of twistor scattering amplitudes suggest an extremely simple picture about the situation. The divergences of the energy momentum currents of Vol and S

_{K}would be non-vanishing only at discrete points at partonic 2-surfaces defining generalized vertices so that minimal surface equations would hold almost everywhere as the original proposal indeed stated.

- The fact that all the known extremals of field equations for S are minimal surfaces conforms with the idea. This might be due to the fact that these extremals are especially easy to construct but could be also true quite generally apart from singular points. The divergences of the energy momentum currents associated with S
_{K}and Vol vanish separately: this follows from the analog of holomorphy reducing the field equations to purely algebraic conditions.

It is essential that Kähler current j

_{K}vanishes or is light-like so that its contraction with the gradients of the imbedding space coordinates vanishes. Second condition is that in transversal degrees of freedom energy momentum tensor is tensor of form (1,1) in the complex sense and second fundamental form consists of parts of type (1,1) and (-1-1). In longitudinal degrees of freedom the trace H^{k}of the second fundamental form H^{k}_{αβ}= D_{β}∂_{α}h^{k}vanishes.

- Minimal surface equations are an analog of massless field equation but one would like to have also the analog of massless particle. The 3-D light-like boundaries between Minkowskian and Euclidian space-time regions are indeed analogs of massless particles as are also the string like word sheets, whose exact identification is not yet fully settled. In any case, they are crucial for the construction of scattering amplitudes in TGD based generalization of twistor Grassmannian approach. At M
^{8}side these points could correspond to singularities at which Galois group of the extension of rationals has a subgroup leaving the point invariant. The points at which roots of polynomial as function of parameters co-incide would serve as an analog.

The intersections of string world sheets with the orbits of partonic 2-surface are 1-D light-like curves X

^{1}_{L}defining fermion lines. The twistor Grassmannian proposal is that the ends of the fermion lines at partonic 2-surfaces defining vertices provide the information needed to construct scattering amplitudes so that information theoretically the construction of scattering amplitudes would reduce to an analog of quantum field theory for point-like particles.

- Number theoretic vision reduces coupling constant evolution to a discrete evolution. This implies that twistor scattering amplitudes for given values of discretized coupling constants involve no radiative corrections. The cuts for the scattering amplitudes would be replaced by sequences of poles. This is unavoidable also because there is number theoretical discretization of momenta from the condition that their components belong to an extension of rationals defining the adele.

- Poles of an analytic function are co-dimension 2 objects. d'Alembert/Laplace equations holding true in Minkowskian/Euclidian signatures express the analogs of analyticity in 4-D case. Co-dimension 2 rule forces to ask whether partonic 2-surfaces defining the vertices and string world sheets could serve analogs of poles at space-time level? In fact, the light-like orbits X
^{3}_{L}of partonic 2-surfaces allow a generalization of 2-D conformal invariance since they are metrically 2-D so that X^{3}_{L}and string world sheets could serve in the role of poles.

X

^{3}_{L}could be seen as analogs of orbits of bubbles in hydrodynamical flow in accordance with the hydrodynamical interpretations. Particle reactions would correspond to fusions and decays of these bubbles. Strings would connect these bubbles and give rise to tensor networks and serve as space-time correlates for entanglement. Reaction vertices would correspond to common ends for the incoming and outgoing bubbles. They would be analogous to the lines of Feynman diagram meeting at vertex: now vertex would be however 2-D partonic 2-surface.

- What can one say about the singularities associated with the light-like orbits of partonic 2-surfaces? The divergence of the Kähler part T
_{K}of energy momentum current T is proportional to a sum of contractions of Kähler current j_{K}with gradients ∇ h^{k}of H coordinates. j_{K}need not be vanishing: it is enough that its contraction with ∇ h^{k}vanishes and this is true if j_{K}is light-like. This is the case for so called massless extremals (MEs). For the other known extremals j_{K}vanishes.

Could the Kähler current j

_{K}be light-like and non-vanishing and singular at X^{3}_{L}and at string world sheets? This condition would provide the long sought-for precise physical identification of string world sheets. Minimal surface equations would hold true also at these surface. Even more: j_{K}could be non-vanishing and thus also singular only at the 1-D intersections X^{1}_{L}of string world sheets with X^{3}_{L}- I have called these curves fermionic lines?

What it means that j

_{K}is singular - that is has 2-D delta function singularity at string world sheets? j_{K}is defined as divergence of the induced Kähler form J so that one can use the standard definition of derivative to define j_{K}at string world sheet as the limiting value j_{K}^{α}= (Div_{+-}J)^{α}= lim_{Δ xn→ 0}(J_{+}^{α n}- J_{-}^{α n})/Δ x^{n}, where x^{n}is a coordinate normal to the string world sheet. If J is not light-like, it gives rise to isometry currents with non-vanishing divergence at string world sheet. This current should be light like to guarantee that energy momentum currents are divergenceless. This is guaranteed if the isometry currents T^{&n; A}are continuous through the string world sheet.

- If the light-like j
_{K}at partonic orbits is localized at fermionic lines X^{1}_{L}, the divergences of energy momentum currents could be non-vanishing and singular only at the vertices defined at partonic 2-surfaces at which fermionic lines X^{1}_{L}meet. The divergences of energy momentum tensors T_{K}of S_{K}and T_{Vol}of Vol would be non-vanishing only at these vertices. They should of course cancel each other: Div T_{K}=-Div T_{Vol}.

- Div T
_{K}should be non-vanishing and singular only at the intersections of string world sheets and partonic 2-surfaces defining the vertices as the ends of fermion lines. How to translate this statement to a more precise mathematical form? How to precisely define the notions of divergence at the singularity?

The physical picture is that there is a sharing of conserved isometry charges of the incoming partonic orbit i=1 determined T

_{K}between 2 outgoing partonic orbits labelled by j=2,3 . This implies charge transfer from i=1 to the partonic orbits j=2,3 such that the sum of transfers sum up to to the total incoming charge. This must correspond to a non-vanishing divergence proportional to delta function. The transfer of the isometry charge for given pair i,j of partonic orbits that is Div_{i→ j}T_{K}must be determined as the limiting value of the quantity Δ_{i→ j}T_{K}^{α,A}/Δ x^{α}as Δ x^{α}approaches zero. Here Δ_{i→ j}T_{K}^{α,A}is the difference of the components of the isometry currents between partonic orbits i and j at the vertex. The outcome is proportional delta function.

- Similar description applies also to the volume term. Now the trace of the second fundamental form would have delta function singularity coming from Div T
_{K}. The condition Div T_{K}= -Div T_{Vol}would bring in the dependence of the boundary conditions on coupling parameters so that space-time surface would depend on the coupling constants in accordance with quantum-classical correspondence. The manner how the coupling constants make themselves visible in the properties of space-time surface would be extremely delicate.

^{8}and H sides of M

^{8}-H duality.

- M
^{8}dynamics based on algebraic equations for space-time surfaces leads to the proposal that scattering amplitudes can be constructed using the data only at the points of space-time surface with M^{8}coordinates in the extension of the rationals defining the adele. I call this discrete set of points cognitive representation.

- At H side the information theoretic interpretation would be that all information needed to construct scattering amplitudes would come from points at which the divergences of the energy momentum tensors of S
_{K}and Vol are non-vanishing and singular.

See the article The Recent View about Twistorialization in TGD Framework or the shorter article Further comments about classical field equations in TGD framework, or the chapter chapterwith the same title.

For a summary of earlier postings see Latest progress in TGD.

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