Derivatives of powers of the Japanese bracket #
On a real inner product space E, write ⟨x⟩ = (1 + ‖x‖ ^ 2) ^ (1 / 2) for the Japanese bracket.
For every real r and every k, the k-th derivative of ⟨x⟩ ^ (2r) = (1 + ‖x‖ ^ 2) ^ r decays
like the bracket power of order 2r - k:
‖D^k (1 + ‖x‖ ^ 2) ^ r‖ ≤ C (1 + ‖x‖ ^ 2) ^ (r - k / 2).
Each derivative gains one power of ⟨x⟩⁻¹; this is the statement that ⟨x⟩ ^ (2r) is a symbol of
order 2r in Hörmander's sense. The same holds for ⟪x, v⟫ (1 + ‖x‖ ^ 2) ^ r, of order 2r + 1.
For r ≤ 0, and for r ≤ -1 / 2 in the case of ⟪x, v⟫ (1 + ‖x‖ ^ 2) ^ r, these symbols have
nonpositive order. Those are the estimates that make the symbols of the Bessel potentials of
nonpositive order, and of first derivatives composed with the Bessel potential of order -1,
multipliers of Mihlin type, and so bounded on Lᵖ for 1 < p < ∞.
The derivative of (1 + ‖x‖ ^ 2) ^ r is (1 + ‖x‖ ^ 2) ^ (r - 1) times the linear map
2r ⟪x, ·⟫, and a smooth function times a continuous linear map gains half a power of
1 + ‖x‖ ^ 2 in its derivative bounds
(ContinuousLinearMap.exists_norm_iteratedFDeriv_smul_le_one_add_norm_sq_rpow). The bounds follow
by induction on k. Rescaling the argument by c ≠ 0 changes 1 + ‖x‖ ^ 2 by at most a constant
factor, so (1 + ‖c x‖ ^ 2) ^ r satisfies the same bounds.
Main declarations #
TauCeti.exists_norm_iteratedFDeriv_one_add_norm_sq_rpow_le: the derivative bounds for(1 + ‖x‖ ^ 2) ^ r.TauCeti.exists_norm_iteratedFDeriv_inner_mul_one_add_norm_sq_rpow_le: the derivative bounds for⟪x, v⟫ (1 + ‖x‖ ^ 2) ^ r.TauCeti.exists_norm_iteratedFDeriv_one_add_norm_sq_rpow_mul_le: the derivative bounds for a bracket power times a smooth cutoffχlocalized where1 + ‖x‖ ^ 2 ≍ R ^ 2and adapted to the scaleR: the product isO(R ^ s / R ^ k)in itsk-th derivative.TauCeti.one_add_norm_sq_rpow_half_le_one_add_norm_rpow: forp ≥ 0,(1 + ‖x‖ ^ 2) ^ (p / 2) ≤ (1 + ‖x‖) ^ p.TauCeti.exists_one_add_norm_smul_sq_rpow_le,TauCeti.exists_norm_iteratedFDeriv_one_add_norm_smul_sq_rpow_le: the bracket power of a rescaled argumentc xand its derivative bounds.ContinuousLinearMap.exists_norm_iteratedFDeriv_comp_left_le_one_add_norm_sq_rpow: composing on the left with a continuous linear map preserves bracket bounds on derivatives.
References #
- L. Grafakos, Modern Fourier Analysis, 3rd ed., Section 1.3 (Bessel potentials).
- M. Taylor, Partial Differential Equations I, Chapter 4, §1.
A continuous linear map grows like (1 + ‖x‖ ^ 2) ^ (1 / 2), its derivative is constant, and
its higher derivatives vanish: ‖D^j L x‖ ≤ ‖L‖ (1 + ‖x‖ ^ 2) ^ ((1 - j) / 2) for every j.
If the first k derivatives of a smooth function g satisfy the bracket bounds
‖D^i g x‖ ≤ C (1 + ‖x‖ ^ 2) ^ (ρ - i / 2), then the k-th derivative of g x • L x, for a
continuous linear map L, satisfies the bracket bound of order ρ + 1 / 2.
Composing on the left with a continuous linear map L preserves a bracket bound
‖D^k g x‖ ≤ C (1 + ‖x‖ ^ 2) ^ ρ, with the constant multiplied by ‖L‖.
Where a R ^ 2 ≤ 1 + ‖ξ‖ ^ 2 ≤ b R ^ 2, every power (1 + ‖ξ‖ ^ 2) ^ (u / 2) of the Japanese
bracket is at most max (a ^ (u / 2)) (b ^ (u / 2)) R ^ u.
The derivative of (1 + ‖x‖ ^ 2) ^ r is (1 + ‖x‖ ^ 2) ^ (r - 1) times 2r ⟪x, ·⟫.
Derivative bounds for powers of the Japanese bracket. For every real r and every k,
‖D^k (1 + ‖x‖ ^ 2) ^ r‖ ≤ C (1 + ‖x‖ ^ 2) ^ (r - k / 2): each derivative of
(1 + ‖x‖ ^ 2) ^ r gains a factor (1 + ‖x‖ ^ 2) ^ (-1 / 2).
Derivative bounds for a linear function times a bracket power. For every v, every real
r and every k, ‖D^k (⟪x, v⟫ (1 + ‖x‖ ^ 2) ^ r)‖ ≤ C (1 + ‖x‖ ^ 2) ^ (r + 1 / 2 - k / 2).
Bessel-weighted dyadic cutoffs are symbols of order s at scale R. Let a > 0, b,
N and B : ℕ → ℝ. There is a constant K ≥ 0 with the following property. Let R > 0 and let
χ be a smooth real function such that a R ^ 2 ≤ 1 + ‖ξ‖ ^ 2 ≤ b R ^ 2 on the support of χ and
‖D^k χ‖ ≤ B k / R ^ k for k ≤ N. Then ‖D^k ((1 + ‖·‖ ^ 2) ^ (s / 2) χ)‖ ≤ K R ^ s / R ^ k for
k ≤ N.
Derivative bounds for a rescaled bracket power. For c ≠ 0, every real r and every
k, ‖D^k (1 + ‖c x‖ ^ 2) ^ r‖ ≤ C (1 + ‖x‖ ^ 2) ^ (r - k / 2).