Smooth functions are dense in W^{1,p}(Ω) (Meyers–Serrin) #
For 1 ≤ p < ∞ and an arbitrary open set Ω of a finite-dimensional real inner product
space, the elements of W^{1,p}(Ω) with a representative which is smooth on Ω are dense in
W^{1,p}(Ω), in the full Sobolev norm. In other words H = W: the closure of
C^∞(Ω) ∩ W^{1,p}(Ω) is all of W^{1,p}(Ω). No boundedness and no regularity of the boundary
of Ω is assumed.
The approximants are smooth on Ω but need not be smooth up to its boundary, nor compactly
supported in Ω: on standard nontrivial bounded domains (for example, Euclidean balls in positive
dimension), W^{1,p}_0(Ω) is a proper subspace, so test functions are not dense. On the whole
space, density of globally smooth representatives at every order is
TauCeti.Wkp.dense_contDiff_representatives.
The argument #
Take a decomposition of unity (ζ j) of Ω by test functions, together with cutoffs χ j equal
to one on the support of ζ j and locally finite in Ω
(IsOpen.exists_contDiff_decomposition_cutoff). Each piece ζ j u is compactly supported in Ω,
so it lies in W^{1,p}_0(Ω) (TauCeti.W1p.contDiffSMul_mem_w1p0Submodule_of_hasCompactSupport) and
is approximated by a test function ψ j to within ε 2^{-j}; cutting off, χ j ψ j still
approximates ζ j u = χ j ζ j u, and now has support where χ j does. The sum f = ∑ j, χ j ψ j
is locally finite in Ω, hence smooth there.
The series ∑ j, ζ j u need not converge to u in W^{1,p}(Ω): its partial sums are cutoffs
of u, and those converge to u only for u ∈ W^{1,p}_0(Ω). So the comparison with u is made
through the corrections instead. These are absolutely summable in the Banach space W^{1,p}(Ω),
to some w of norm at most ε / 2; after passing to a subsequence, representatives of their
partial sums converge almost everywhere on Ω to f - u. Hence u + w is within ε of u, and
its value is represented by f.
Main declarations #
TauCeti.W1p.exists_contDiffOn_approximation: everyu ∈ W^{1,p}(Ω)is a Sobolev-norm limit of elements with representatives smooth onΩ.TauCeti.W1p.dense_contDiffOn_representatives: those elements are dense inW^{1,p}(Ω).
References #
- N. G. Meyers, J. Serrin, H = W, Proc. Nat. Acad. Sci. U.S.A. 51 (1964), 1055–1056.
- L. C. Evans, Partial Differential Equations, §5.3.2, Theorem 2.
Meyers–Serrin approximation in W^{1,p}(Ω). For 1 ≤ p < ∞ and an arbitrary open set
Ω, every u ∈ W^{1,p}(Ω) is a limit, in the full Sobolev norm, of elements whose values are
represented by functions smooth on Ω. No boundedness or boundary regularity of Ω is
assumed.
Meyers–Serrin: H = W in W^{1,p}(Ω). For 1 ≤ p < ∞ and an arbitrary open set Ω,
the elements of W^{1,p}(Ω) represented by functions smooth on Ω are dense in W^{1,p}(Ω),
in the full Sobolev norm.