Summary
In mathematical analysis, Hölder's inequality, named after Otto Hölder, is a fundamental inequality between integrals and an indispensable tool for the study of Lp spaces. The numbers p and q above are said to be Hölder conjugates of each other. The special case p = q = 2 gives a form of the Cauchy–Schwarz inequality. Hölder's inequality holds even if 1 is infinite, the right-hand side also being infinite in that case. Conversely, if f is in Lp(μ) and g is in Lq(μ), then the pointwise product fg is in L1(μ). Hölder's inequality is used to prove the Minkowski inequality, which is the triangle inequality in the space Lp(μ), and also to establish that Lq(μ) is the dual space of Lp(μ) for p ∈ . Hölder's inequality (in a slightly different form) was first found by . Inspired by Rogers' work, gave another proof as part of a work developing the concept of convex and concave functions and introducing Jensen's inequality, which was in turn named for work of Johan Jensen building on Hölder's work. The brief statement of Hölder's inequality uses some conventions. In the definition of Hölder conjugates, 1/∞ means zero. If p, q ∈ , then p and q stand for the (possibly infinite) expressions If p = ∞, then ∞ stands for the essential supremum of , similarly for ∞. The notation p with 1 ≤ p ≤ ∞ is a slight abuse, because in general it is only a norm of f if p is finite and f is considered as equivalence class of μ-almost everywhere equal functions. If f ∈ Lp(μ) and g ∈ Lq(μ), then the notation is adequate. On the right-hand side of Hölder's inequality, 0 × ∞ as well as ∞ × 0 means 0. Multiplying a > 0 with ∞ gives ∞. As above, let f and g denote measurable real- or complex-valued functions defined on S. If 1 is finite, then the pointwise products of f with g and its complex conjugate function are μ-integrable, the estimate and the similar one for fg hold, and Hölder's inequality can be applied to the right-hand side. In particular, if f and g are in the Hilbert space L2(μ), then Hölder's inequality for p = q = 2 implies where the angle brackets refer to the inner product of L2(μ).
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