Solution.
Let g be a Lebesgue measurable function on R satisfying conditions (ii) and (iii). Then
∫R∣g(x)∣dx=∫{∣x∣≤1}∣g(x)∣dx+∫{∣x∣>1}∣g(x)∣dx=∫{∣x∣≤1}∩{∣g(x)∣≥1}∣g(x)∣dx+∫{∣x∣≤1}∩{∣g(x)∣<1}∣g(x)∣dx+∫{∣x∣>1}∣g(x)∣dx≤∫{∣x∣≤1}∩{∣g(x)∣≥1}∣g(x)∣2dx+∫{∣x∣≤1}dx+∫{∣x∣>1}∣x∣∣g(x)∣dx≤200+2<∞,
so g∈L1. Hence, fn∈L1 for all n. By Fatou's lemma, we also see that
∫R∣x∣∣f(x)∣dx≤n→∞liminf∫R∣x∣∣fn(x)∣dx≤100∫R∣f(x)∣2dx≤n→∞liminf∫R∣fn(x)∣2dx≤100,
so f satisfies the same conditions, i.e., f∈L1 as well. To prove L1 convergence, fix ε>0. Then observe that
∫{∣x∣≥R}∣fn(x)∣dx≤∫{∣x∣≥R}∣x∣∣x∣∣fn(x)∣dx≤R100,
and this inequality is true with fn replaced with f as well. Thus, we may pick R>0 large enough so that ∫{∣x∣≥R}∣fn(x)∣dx<ε and ∫{∣x∣≥R}∣f(x)∣dx<ε. On the finite measure set B(0,R), we may apply Egorov's theorem, since fn→f almost everywhere. Hence, we get E⊆B(0,R) such that fn→f uniformly on B(0,R)∖E and with m(E)<ε. Thus, if n is large enough, then ∣fn−f∣<2Rε on B(0,R)∖E, and so
∫R∣fn−f∣dx≤∫B(0,R)∣fn−f∣dx+∫{∣x∣≥R}∣fn∣dx+∫{∣x∣≥R}∣f∣dx≤∫E∣fn−f∣dx+∫B(0,R)∖E∣fn−f∣dx+2ε≤∥fn−f∥L2m(E)1/2+3ε≤ε1/2(∥fn∥L2+∥f∥L2)+3ε≤20ε1/2+3ε,
so ∥fn−f∥L1→0.
To see that (2) is necessary, consider fn(x)=f(x)=∣x∣−1χB(0,1). Then these satisfy (1) trivially and satisfy (2) since ∣x∣∣fn(x)∣=χB(0,1), which certainly has integral bounded by 100. Moreover, it does not satisfy (3) since fn∈/L2. However, fn∈/L1, since ∣x∣−1 is not integrable near the origin, so the conclusion fails.
Similarly, to see that (3) is necessary, let fn(x)=f(x)=∣x∣−1χ{∣x∣≥1}. This it's clear that (1) and (3) are satisfied, but (2) is not satisfied since ∣x∣∣fn(x)∣=χ{∣x∣≥1}, which has infinite mass. As before, fn∈/L1, so the conclusion fails.