The parity symmetry of the period relation and Hecke equivariance of r_f^± #
Let ε = !![-1, 0; 0, 1]. Conjugation A ↦ ε A ε sends a determinant-n matrix (a b; c d) to
(a -b; -c d), again of determinant n, and descends to an involution of the projective matrix
module ℳₙ. It normalizes the data of Popa and Zagier's period relation
(A) (1 - S)·ξ - Tₙ^∞·(1 - S) ∈ (1 - T)·ℛₙ:
ε S ε = -S acts on ℳₙ as S, on the left and on the right; ε T ε = T⁻¹, so the ideal
(1 - T)·ℛₙ is preserved; and each upper-triangular representative (a b; 0 d) of Γ \ ℳₙ goes
to (a -b; 0 d), which lies in the ⟨T⟩-orbit of another representative, so the conjugate of
Tₙ^∞ has the same ⟨T⟩-orbit sums as Tₙ^∞. Hence the conjugate of a solution of (A) is again
a solution.
The conjugate of ξ acts on binary forms by P ↦ ((P ∣ ε) ∣ ξ) ∣ ε. Every solution of (A) acts
on the period polynomials of level-one cusp forms as the Hecke operator Tₙ (Popa–Zagier,
Proposition 2). Applying this to ξ and to its conjugate shows that the action of ξ commutes
with the parity involution P(X, Y) ↦ P(-X, Y) on period polynomials of cusp forms:
(r_f ∣ ε) ∣ ξ = r_{Tₙ f} ∣ ε. Consequently the even and odd period polynomials are
Hecke-equivariant, r_f^± ∣ ξ = r_{Tₙ f}^±: the maps f ↦ r_f^± from S_k(SL(2, ℤ)) to W_w^±
intertwine Tₙ with the action of any solution of (A), such as Popa and Zagier's explicit
element.
Main definitions #
TauCeti.TraceFormulaMatrix.parityConj: the conjugateε A εof a determinant-nmatrix.TauCeti.TraceFormulaMatrixModule.parityConj: the induced involution ofℳₙ.
Main results #
TauCeti.TraceFormulaMatrixModule.mapDomainLinearMap_parityConj_upperTriangularSum_sub_mem: the conjugate ofTₙ^∞is congruent toTₙ^∞modulo(1 - T)·ℛₙ.TauCeti.TraceFormulaMatrixModule.PeriodRelation.mapDomainLinearMap_parityConj: the conjugate of a solution of the period relation (A) is a solution.TauCeti.TraceFormulaMatrixModule.periodAction_mapDomainLinearMap_parityConj: the conjugate ofξacts on binary forms byP ↦ ((P ∣ ε) ∣ ξ) ∣ ε.TraceFormulaMatrixModule.PeriodRelation.periodAction_binaryFormRep_parity_periodPolynomial:(r_f ∣ ε) ∣ ξ = r_{Tₙ f} ∣ εfor every solutionξof (A).TauCeti.TraceFormulaMatrixModule.PeriodRelation.periodAction_evenPeriodPolynomialandTauCeti.TraceFormulaMatrixModule.PeriodRelation.periodAction_oddPeriodPolynomial:r_f^± ∣ ξ = r_{Tₙ f}^±.
References #
- A. Popa and D. Zagier, An elementary proof of the Eichler–Selberg trace formula, J. Reine Angew. Math. 762 (2020), 105–122, arXiv:1711.00327, §§1–2. The period relation (A) is stated in §1 and Proposition 2 is in §2.
The conjugate ε A ε of a determinant-n matrix A = (a b; c d) by the parity matrix
ε = !![-1, 0; 0, 1]: the matrix (a -b; -c d), again of determinant n.
Instances For
The underlying matrix of TraceFormulaMatrix.parityConj A is ε A ε.
Conjugation by the parity matrix commutes with negation.
The involution of the projective matrix module ℳₙ induced by conjugation A ↦ ε A ε by the
parity matrix ε = !![-1, 0; 0, 1].
Instances For
On a representative, the involution of ℳₙ is conjugation by the parity matrix.
Conjugation by the parity matrix is an involution of ℳₙ.
Conjugation by the parity matrix is an involution of ℳₙ.
ε S ε = -S, so conjugation by the parity matrix commutes with left multiplication by S.
ε T^m ε = T^(-m), so conjugation by the parity matrix turns left multiplication by T ^ m
into left multiplication by T ^ (-m).
ε T ε = T⁻¹, so conjugation by the parity matrix turns left multiplication by T into left
multiplication by T⁻¹.
ε S ε = -S, so conjugation by the parity matrix commutes with right multiplication by S.
The conjugate of Tₙ^∞ #
The conjugate of Tₙ^∞ by the parity matrix is Tₙ^∞ modulo (1 - T)·ℛₙ. Conjugation
sends the representative (a b; 0 d) of ℳₙ^∞ to (a -b; 0 d), which lies in the ⟨T⟩-orbit of
the representative (a b'; 0 d) with b' ≡ -b mod d.
The parity conjugate of a solution of the period relation is a solution. If ξ satisfies
Popa–Zagier's period relation (A), then so does its image under conjugation M ↦ ε M ε by
ε = !![-1, 0; 0, 1].
The action on binary forms #
The parity conjugate acts by conjugating with the parity involution. The image of ξ
under M ↦ ε M ε acts on binary forms of even degree by P ↦ ((P ∣ ε) ∣ ξ) ∣ ε.
Hecke equivariance of the even and odd period polynomials #
The Hecke action commutes with the parity involution on period polynomials. Let n ≥ 1
and let ξ be a solution of the period relation (A). For every level-one cusp form f of weight
w + 2, (r_f ∣ ε) ∣ ξ = r_{Tₙ f} ∣ ε, where ε = !![-1, 0; 0, 1] acts by
P(X, Y) ↦ P(-X, Y) and Tₙ = TauCeti.heckeTCuspLevelOne (w + 2) n.
Hecke equivariance of the even period polynomial. Let n ≥ 1 and let ξ be a solution of
the period relation (A). For every level-one cusp form f of weight w + 2,
r_f^+ ∣ ξ = r_{Tₙ f}^+, with Tₙ = TauCeti.heckeTCuspLevelOne (w + 2) n.
Hecke equivariance of the odd period polynomial. Let n ≥ 1 and let ξ be a solution of
the period relation (A). For every level-one cusp form f of weight w + 2,
r_f^- ∣ ξ = r_{Tₙ f}^-, with Tₙ = TauCeti.heckeTCuspLevelOne (w + 2) n.