Spring 2012 - Problem 4

Lp spaces

Let S={fL1(R3)fdx=0}S = \set{f \in L^1\p{\R^3} \mid \int f \,\diff{x} = 0}.

  1. Show that SS is closed in the L1L^1 topology.
  2. Show that SL2(R3)S \cap L^2\p{\R^3} is a dense subset of L2(R3)L^2\p{\R^3}.
Solution.
  1. Let {fn}nS\set{f_n}_n \subseteq S be a sequence such that fnff_n \to f in L1L^1. Then

    fdx=ffndxffnL1n0,\abs{\int f \,\diff{x}} = \abs{\int f - f_n \,\diff{x}} \leq \norm{f - f_n}_{L^1} \xrightarrow{n\to\infty} 0,

    so fSf \in S.

  2. Compactly supported functions L2L^2 functions are dense in L2(R3)L^2\p{\R^3}, so it suffices to prove that SL2(R3)S \cap L^2\p{\R^3} is dense for such functions.

    Let fL2(R3)f \in L^2\p{\R^3} have compact support. Set I=fdxI = \int f \,\diff{x} and R>0R > 0 be such that the support of ff is contained in B(0,R)B\p{0, R}. Let σ\sigma denote the surface measure on the unit ball S2S^2 so that S2dσ=4π\int_{S^2} \diff\sigma = 4\pi. Thus, by polar coordinates,

    m(B(0,a))=0aS2r2dσdr=4πr33.m\p{B\p{0, a}} = \int_0^a \int_{S^2} r^2 \,\diff\sigma \,\diff{r} = \frac{4\pi r^3}{3}.

    Fix ε>0\epsilon > 0. Set g=fg = f on B(0,R)B\p{0, R} and for RxMR \leq \abs{x} \leq M (where M>RM > R will be chosen later), let g=Iεg = -I\epsilon (it's only important that gg has the opposite sign of II on this interval). Then

    gdx=fdxB(0,M)B(0,R)Iεdx=I4πIε3(M3R3).\int g \,\diff{x} = \int f \,\diff{x} - \int_{B\p{0, M} \setminus B\p{0, R}} I\epsilon \,\diff{x} = I - \frac{4\pi I\epsilon}{3}\p{M^3 - R^3}.

    Pick M=(R3+34πε)1/3M = \p{R^3 + \frac{3}{4\pi\epsilon}}^{1/3}, i.e., so that gdx=0\int g \,\diff{x} = 0. Thus, gSg \in S and because fL2(R3)f \in L^2\p{\R^3} and gg is bounded on RxMR \leq \abs{x} \leq M, gL2(R3)g \in L^2\p{\R^3} as well. Finally,

    fgL22=B(0,M)B(0,R)I2ε2dx=m(B(0,M)B(0,R))I2ε2=4π(M3R3)3I2ε2=I2ε.\begin{aligned} \norm{f - g}_{L^2}^2 &= \int_{B\p{0, M} \setminus B\p{0, R}} I^2\epsilon^2 \,\diff{x} \\ &= m\p{B\p{0, M} \setminus B\p{0, R}} I^2\epsilon^2 \\ &= \frac{4\pi\p{M^3 - R^3}}{3} I^2\epsilon^2 \\ &= I^2\epsilon. \end{aligned}

    Since II is independent of ε\epsilon, we may send ε0\epsilon \to 0, and that gives the claim.