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Recipe

Test whether a norm comes from an inner product

Use when: you have two specific functions f,g and a candidate norm, and need to know whether that norm could ever support orthogonal projection

Goal: a verified answer, backed by one concrete check, on whether an inner product could possibly sit behind this norm

Taught in Why L2 is the right space for Fourier series

  1. 1

    For f and g, compute \lVert f\rVert^2 and \lVert g\rVert^2 under the candidate norm.

    Example

    Let f(t)=t and g(t)=1 on [-1,1], tested under \lVert\cdot\rVert_2. Then \lVert f\rVert_2^2=\displaystyle\int_{-1}^1t^2\,dt=\frac23 and \lVert g\rVert_2^2=\displaystyle\int_{-1}^1 1\,dt=2.

    Why: these two numbers, doubled and added, are exactly the identity's right-hand side.

  2. 2

    Form f+g and f-g, then compute \lVert f+g\rVert^2 and \lVert f-g\rVert^2 under that same norm.

    Example

    f+g=t+1 and f-g=t-1, so \lVert f+g\rVert_2^2=\displaystyle\int_{-1}^1(t+1)^2\,dt=\frac83, and by the matching computation \lVert f-g\rVert_2^2=\frac83 as well.

    Why: these two numbers, added together, are exactly the identity's left-hand side, using the identical norm as Step 1.

  3. 3

    Add the two Step 2 numbers for the left side, and double-and-add the two Step 1 numbers for the right side.

    Example

    Left: \frac83+\frac83=\frac{16}3. Right: 2\left(\frac23\right)+2(2)=\frac43+4=\frac{16}3. The two sides match exactly.

    Why: this sum-of-squares equation is the literal statement of the parallelogram law, not an approximation of it.

  4. 4

    A mismatch is decisive: it rules the norm out completely, for every pair of functions, forever. A match on one pair proves nothing beyond that single pair.

    Example

    Under \lVert\cdot\rVert_\infty, take f(t)=1 and g(t)=+1 for t>0, -1 for t<0, both on [-1,1]. Then \lVert f+g\rVert_\infty^2+\lVert f-g\rVert_\infty^2=4+4=8, while 2\lVert f\rVert_\infty^2+2\lVert g\rVert_\infty^2=2+2=4. The mismatch alone rules \lVert\cdot\rVert_\infty out.

    • the two sides disagree — the norm fails the parallelogram law and can never come from any inner product.
    • the two sides agree — this pair is consistent with an inner product, but a general proof is still needed to conclude the law always holds.

    Why: one failing pair is airtight evidence, while one confirming pair only ever confirms itself.

Common mistakes

  • Mixing two different norms across the four quantities, such as computing \lVert f\rVert in L^2 but \lVert f+g\rVert in L^\infty.
  • Forgetting to square each norm before adding; the identity uses squared norms throughout, not the plain norms.
  • Treating one confirming pair as proof the law holds for every pair under that norm.
  • Concluding a norm supports orthogonal projection just because a single parallelogram check happened to succeed.