PhysLean Documentation

PhysLean.QFT.AnomalyCancellation.PureU1.Even.Parameterization

Parameterization in even case #

Given maps g : Fin n.succ → ℚ, f : Fin n → ℚ and a : ℚ we form a solution to the anomaly equations. We show that every solution can be got in this way, up to permutation, unless it, up to permutation, lives in the plane spanned by the first part of the basis vector.

The main reference is:

def PureU1.Even.parameterizationAsLinear {n : } (g : Fin n.succ) (f : Fin n) (a : ) :

Given coefficients g of a point in P and f of a point in P!, and a rational, we get a rational a ∈ ℚ, we get a point in (PureU1 (2 * n.succ)).AnomalyFreeLinear, which we will later show extends to an anomaly free point.

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    theorem PureU1.Even.parameterizationCharge_cube {n : } (g : Fin n.succ) (f : Fin n) (a : ) :
    def PureU1.Even.parameterization {n : } (g : Fin n.succ) (f : Fin n) (a : ) :
    (PureU1 (2 * n.succ)).Sols

    The construction of a Sol from a Fin n.succ → ℚ, a Fin n → ℚ and a .

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      def PureU1.Even.GenericCase {n : } (S : (PureU1 (2 * n.succ)).Sols) :

      A proposition on a solution which is true if accCubeTriLinSymm (P g, P g, P! f) ≠ 0. In this case our parameterization above will be able to recover this point.

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        def PureU1.Even.SpecialCase {n : } (S : (PureU1 (2 * n.succ)).Sols) :

        A proposition on a solution which is true if accCubeTriLinSymm (P g, P g, P! f) = 0.

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          theorem PureU1.Even.generic_case {n : } {S : (PureU1 (2 * n.succ)).Sols} (h : GenericCase S) :
          ∃ (g : Fin n.succ) (f : Fin n) (a : ), S = parameterization g f a