The Japanese bracket in L² and the L¹ bound by a weighted L² norm #
Let V be a finite-dimensional real normed space of dimension d. For 2s > d the negative
power (1 + ‖x‖ ^ 2) ^ (-s / 2) of the Japanese bracket is square integrable for every additive
Haar measure (TauCeti.memLp_rpow_neg_one_add_norm_sq), since its square is the integrable
function (1 + ‖x‖ ^ 2) ^ (-2s / 2) (integrable_rpow_neg_one_add_norm_sq). For every s, the
Cauchy–Schwarz inequality gives
‖v‖₁ ≤ ‖(1 + ‖·‖ ^ 2) ^ (-s / 2)‖₂ ‖(1 + ‖·‖ ^ 2) ^ (s / 2) v‖₂
(TauCeti.eLpNorm_one_le_eLpNorm_rpow_neg_one_add_norm_sq_mul_eLpNorm_one_add_norm_sq_rpow_smul).
Together these bound the L¹ norm of a function by a weighted L² norm when 2s > d. Applied
to the Fourier transform of a function in the Bessel-potential space H^s, whose H^s norm is
the weighted L² norm of its Fourier transform, this is the estimate behind the Sobolev embedding
H^s ⊆ C₀ and the algebra property of H^s for s > d / 2.
References #
- G. B. Folland, Real Analysis, 2nd ed., §9.3.
For 2s > dim V the function (1 + ‖x‖ ^ 2) ^ (-s / 2) is square integrable.
The L¹ norm is bounded by a weighted L² norm. For every s and every function v,
‖v‖₁ ≤ ‖(1 + ‖·‖ ^ 2) ^ (-s / 2)‖₂ ‖(1 + ‖·‖ ^ 2) ^ (s / 2) v‖₂. The first factor is finite
when 2s > dim V (TauCeti.memLp_rpow_neg_one_add_norm_sq).