TrueLevelBasis #
The circle defect rhoh(w) = ||1+w| - 1|.
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positiveTrigonometricPolynomial: positive Trigonometric Polynomial.
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circleModulusDefect: circle Modulus Defect.
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Core Basis Objects #
The true Hermite basis vector at level k, written directly as the explicit
finite z/conj z expansion used downstream.
The raising/lowering-operator derivation is only bookkeeping motivation; the public API stays explicit and finitary.
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The distinguished lowest vector in level k.
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The closed span of the true Hermite level-k basis.
An element G belongs to Hk k when its canonical Hermite-coefficient
expansion converges pointwise to G and its weighted square norm is
integrable. Equivalently, Hk k is the weighted-L² closure of
span {Φₖ,ₙ} together with the pointwise Hermite expansion data.
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A finite Hermite sum sum_{n < D} a_n Phi_{k,n}.
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- HermitekLEAN.finiteHermiteSum k a z = ∑ n : Fin D, a n * HermitekLEAN.Phi k (↑n) z
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The canonical coefficient extractor for the true level basis.
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- HermitekLEAN.hermiteCoeff k G n = HermitekLEAN.weightedInner G (HermitekLEAN.Phi k n)
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The partial Hermite sum with the first J + 1 canonical coefficients of G.
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- HermitekLEAN.truncate k J G = HermitekLEAN.finiteHermiteSum k fun (n : Fin (J + 1)) => HermitekLEAN.hermiteCoeff k G ↑n
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The finitely supported circle coefficient map attached to finite Hermite data.
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- HermitekLEAN.finiteCircleCoeff k r a n = if h : n < D then a ⟨n, h⟩ * ↑(HermitekLEAN.qkn k n r) else 0
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The finite Fourier polynomial on the circle attached to a finite Hermite sum.
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The finite circle polynomial built from the truncated coefficient vector of G.
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- HermitekLEAN.truncCirclePoly k r J G = HermitekLEAN.finiteCirclePoly k r fun (n : Fin (J + 1)) => HermitekLEAN.hermiteCoeff k G ↑n
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Explicit and Polar Formulas #
Explicit finite expansion for the true Hermite basis vector Phi k n.
Finite-First Basis API #
Helpers for the diagonal case of phi_orthonormal #
Double-sum identity for phi_orthonormal diagonal case #
Inner products of finite Hermite sums are finite coefficient inner products.
The weighted norm square of a finite Hermite sum is the coefficient ℓ² norm square.
Weighted norms are homogeneous under scalar multiplication.
Weighted defect norms are homogeneous under scalar multiplication.
Every finite Hermite sum belongs to the true level space.
The canonical coefficient extractor recovers the coefficients of a finite Hermite sum.
The zeroth coefficient is the inner product against the lowest basis vector.
Orthogonality to Phi k 0 is equivalent to vanishing zeroth Hermite coefficient.
The truncation operator is the explicit finite Hermite sum of the first coefficients.
The truncated circle polynomial is the finite circle polynomial of the truncated vector.
Exact finite Parseval identity for Hermite truncations.
Finite Hermite sums admit a finite circle representation.
The finite circle coefficient map vanishes outside the finite frequency range.
The finite circle polynomial is supported in frequencies {0, ..., D - 1}.
If the zeroth coefficient vanishes, the finite circle polynomial has positive-frequency support.
Truncations admit the corresponding finite circle representation.
The truncation circle polynomial is supported in {0, ..., J}.
Orthogonality to Phi k 0 removes the zero frequency from every
truncation circle polynomial.
Circle Parseval identity for truncated Hermite sums.
Basis Bridge #
The formal Hermite expansion attached to a coefficient sequence.
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- HermitekLEAN.hermiteSeries k g z = ∑' (n : ℕ), g n * HermitekLEAN.Phi k n z
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The canonical coefficient extractor recovers the Hermite expansion of any G ∈ H_k.
Compatibility statement: polar/circle representation of an element of H_k.
Canonical circle representation in terms of hermiteCoeff.
Circle Parseval identity for the canonical coefficient sequence.
The canonical circle series has the expected Fourier coefficients.
The finite circle polynomials of G converge in circle L² to the Hermite circle series.
Hermite expansions converge locally uniformly, hence are continuous.
Every element of H_k is continuous.
The modulus defect is bounded by the perturbation norm.