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The relationship between position configuration variables and momentum can first be seen by looking at the diagram I attach. This illustrates a scattering process with 5 input momenta and 5 output momenta. The "blob" is the region with virtual or off shell processes, which can be realized by on shell processes by BCFW recursion. I will ignore that matter for the moment. The momenta labeled with number 1, 2, 3, ..., 10 must all add to zero if we reverse the sign of the outgoing momenta. This is a trick used in working out the S, T, U channels. These momenta can then form a polygon. It is tempting of course to think of the configuration variables as defining the momenta by p1 = x1 - x2, p2 = x2 - x3, and so forth. However, this polygon has a dual polygon, which may be constructed by drawing a line through the mid points of the momentum edgelinks and then finding where these lines intersect. This will be the dual polygon. This dual polygon is then the vectors which represent the position variables of these particles. This is the more sophisticated way of such a representation for it does not rely upon an explicit reference to either set of variables to derive the other, but rather depends upon a duality principle.
In three dimensional space the diagram is more complex and the polygon is replaced with a polytope in three dimensions. Further, since the diagram on the left is really a spacetime diagram, with time running to the right, the polygon is really replaced with a polytope in four dimensions. The fundamental polytopes in four dimensions are the 24-cell, which is self-dual and the 120-cell that is dual to the 600-cell. In order to construct a one to one self duality between momentum and position configuration variables the 24-cell is the obvious model. For systems with more particles than can be represented by a single 24-cell tessellations of 24-cells may then be considered.
The 24-cell is a representation in Hurwitz quaternions of the F_4 exceptional group. The F_4 group shares a relationship with the B_4 = SO(9)
F_4/B_4:1 --- > spin(9) --- > F_{52/16} --- OP^2 --- > 1
And of course spin groups have a double cover to orthogonal groups
1 -- > Z_2 --- > Spin(n) --- > SO(n) --- > 1
The group SO(9) plays an important role with string theory or holography. Physics on an infinite momentum frame, physics observed boosted enormously, reduces the relevant physics to one dimension less, and the observed physics by time dilation is effectively nonrelativistic by time dilation. I illustrate this briefly below. This reduces the 10 dimensions of supergravity to 9, and the symmetry group of this spacetime is then SO(8,1) ~ SO(9).
It is easy to how an extremely boosted system appears nonrelativitstic. We consider the invariant momentum
m^2 = E^2 - p^2,
here with c = 1. The energy is then
E = sqrt{p_x^2 p_y^2 p_z^2 m^2}
We then consider the momentum p_z as enormous, and p_z >> p_x,y. We factor this out with
E = p_z sqrt{1 (p_x^2 p_y^2)/p_z^2 m^2/p_z^2}
Where binomial theorem gives us
E = p_z (p_x^2 p_y^2)/p_z m^2/p_z
The momentum p_z then acts as a time dilation factor approximating a Lorentz factor. We may group all of this to define a new energy or Hamiltonian
H = (E - p_z)p_z = p_x^2 p_y^2 m^2,
where the right hand side of this equation is a nice classical nonrelativistic Hamiltonian. The mass squared then plays the role of a potential energy.