Young's inequality for products can be used to prove Hölder's inequality. It is also used widely to estimate the norm of nonlinear terms in PDE theory, since it allows one to estimate a product of two terms by a sum of the same terms raised to a power and scaled.
Young's inequality for products
Standard version for conjugate Hölder exponents
Equality holds if and only if ap = bq. This form of Young's inequality is a special case of the inequality of weighted arithmetic and geometric means and can be used to prove Hölder's inequality.
An elementary case of Young's inequality is the inequality with exponent 2,
which also gives rise to the so-called Young's inequality with ε (valid for every ε > 0), sometimes called the Peter–Paul inequality . This name refers to the fact that tighter control of the second term is achieved at the cost of losing some control of the first term – one must "rob Peter to pay Paul"
Standard version for increasing functions
For the standard version of the inequality, let f denote a real-valued, continuous and strictly increasing function on [0, c] with c > 0 and f(0) = 0. Let f−1 denote the inverse function of f. Then, for all a ∈ [0, c] and b ∈ [0, f(c)],
with equality if and only if b = f(a).
Generalization using Legendre transforms
This follows immediately from the definition of the Legendre transform. This inequality also holds — in the form a ·b ≤ f(a) + g(b) — if f is a convex function taking a vector argument (Arnold 1989, §14).
- The Legendre transform of f(a) = ap/p is g(b) = bq/q with q such that 1/p + 1/q = 1, and thus Young's inequality for conjugate Hölder exponents mentioned above is a special case.
- The Legendre transform of f(a) = ea – 1 is g(b) = 1 − b + b ln b, hence ab ≤ ea − b + b ln b for all non-negative a and b. This estimate is useful in large deviations theory under exponential moment conditions, because b ln b appears in the definition of relative entropy, which is the rate function in Sanov's theorem.
Young's inequality for convolutions
Suppose f is in Lp(Rd) and g is in Lq(Rd) and
with 1 ≤ p, q, r ≤ ∞. Then
denotes the usual Lp norm.
An example application is that Young's inequality can be used to show that the heat semigroup is a contracting semigroup using the L2 norm (i.e. the Weierstrass transform does not enlarge the L2 norm).
In case p, q > 1 Young's inequality can be strengthened to a sharp form, viz
where the constant cp,q < 1.
- Young, W. H. (1912), "On classes of summable functions and their Fourier series", Proceedings of the Royal Society A 87 (594): 225–229, doi:10.1098/rspa.1912.0076, JSTOR 93236, Zbl 43.1114.12
- Young, W. H. (1912), "On the multiplication of successions of Fourier constants", Proceedings of the Royal Society A 87 (596): 331–339, doi:10.1098/rspa.1912.0086, JSTOR 93120, Zbl 44.0298.02
- Tisdell, Chris (2013), The Peter Paul Inequality, YouTube video on Dr Chris Tisdell's YouTube channel,
- Hardy, G. H.; Littlewood, J. E.; Pólya, G. (1952) , Inequalities, Cambridge Mathematical Library (2nd ed.), Cambridge: Cambridge University Press, ISBN 0-521-05206-8, MR 0046395, Zbl 0047.05302, Chapter 4.8
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- Fournier, John J. F. (1977), "Sharpness in Young's inequality for convolution", Pacific J. Math. 72 (2): 383–397, MR 0461034, Zbl 0357.43002
- Arnold, V. I. (1989), Mathematical Methods of Classical Mechanics (2. ed.), Springer, ISBN 978-0-387-96890-2.
- Witkowski, Alfred (2006), "On Young's inequality", Journal of Inequalities in Pure and Applied Mathematics 7 (5): 3 p., Zbl pre05224679