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LeanPool.CarlsonFunctions.Carlson.TwoVariable.ParameterSymmetry

Interchanging an exponent and a Dirichlet parameter #

The two numerator parameters in the Gauss series are symmetric. We establish this symmetry first near the all-one node vector, then continue in the parameters and in the slit-plane node. This is the R-identity underlying Carlson (1987), (2.12).

Only one monomial survives when the first polynomial node vanishes.

Gauss numerator-parameter symmetry on the entire slit plane, with all complex parameters allowed by reciprocal-Gamma regularization.

A ratio of two right-half-plane numbers cannot lie on the nonpositive real axis.

theorem DirichletTransform.TwoVariable.regCarlsonRSlit_normalize_first (t : ℂ) (b : Fin 2 → ℂ) {x y : ℂ} (hx : 0 < x.re) (hy : 0 < y.re) :
regCarlsonRSlit t b (pair x y) = x ^ t * regCarlsonRSlit t b (pair 1 (y / x))

Normalize the first node, with branch control for arbitrary right-half-plane nodes. The normalized second node need only belong to the slit plane.

theorem DirichletTransform.TwoVariable.regCarlsonRSlit_parameterInterchange (t u v : ℂ) {x y : ℂ} (hx : 0 < x.re) (hy : 0 < y.re) :
regCarlsonRSlit t (pair u v) (pair x y) = x ^ t * regCarlsonRSlit (-v) (pair (u + v + t) (-t)) (pair 1 (y / x))

Exponent-parameter interchange at two right-half-plane nodes, with no parameter restrictions and a slit-plane ratio on the transformed side.

Simultaneously swapping the two parameters and nodes on the slit domain.

theorem DirichletTransform.TwoVariable.regCarlsonRSlit_parameterInterchange_last (t u v : ℂ) {x y : ℂ} (hx : 0 < x.re) (hy : 0 < y.re) :
regCarlsonRSlit t (pair u v) (pair x y) = y ^ t * regCarlsonRSlit (-u) (pair (-t) (u + v + t)) (pair (x / y) 1)

The second form of the exponent-parameter interchange, normalized at the last node.