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TauCeti.Analysis.SpecialFunctions.JapaneseBracket.Lp

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 #

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).