Solution
ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2001/ib/paper-1/17b/solution
Past exam of the mathematics course of the University of Cambridge 2001 ib Paper 1 17B Solution by
Codex 0 Created 2026-09-24 Updated 2026-10-14
First work over a field of characteristic different from two. If a nonzero symmetric bilinear form had for every vector, polarization would givea contradiction. Hence choose with . Every decomposes uniquely aswith the second summand orthogonal to . Induct on the orthogonal complement to obtain a diagonal basis. If the restricted form becomes zero, any basis of that remaining space completes the diagonalization. In this basis the rank of a quadratic form is exactly the number of nonzero diagonal coefficients; the remaining basis vectors span its radical of a bilinear form.
Over the reals, rescale the nonzero basis vectors so the diagonal entries are copies of , copies of and zeros. Define the signature of a quadratic form by , so . To prove it is basis independent, note that is the largest dimension of a linear subspace on which the form is positive-definite. The positive coordinate linear subspace attains dimension ; on any other positive linear subspace, projection to those positive coordinates is injective, since its kernel has nonpositive quadratic value. Thus its dimension is at most . The same argument for the negative form characterizes . This proves Sylvester's law of inertia and that the signature is well-defined.
Let and be positive and negative normalized basis vectors, and let be the radical of a bilinear form. The span of and for is a totally isotropic subspace: all mutual bilinear pairings vanish. Its dimension is . Conversely, project any totally isotropic subspace to the nondegenerate positive-plus-negative quotient. The projected linear subspace is still null, and its projections to both the positive and negative coordinate spaces are injective: a vector with one component zero would have strictly signed quadratic value unless it vanished. Its dimension is therefore at most , while the kernel of the quotient map on has dimension at most . HenceThis proves both construction and sharpness of the maximum dimension of a totally isotropic subspace.
For the five-variable example, the symmetric coefficient matrix isIts cyclic structure makes the vectors , , eigenvectors with eigenvalues . Thus the eigenvalues areTheir product is , and three are positive and two negative. ThereforeThe real and imaginary parts of each conjugate pair of eigenvectors give the corresponding real two-dimensional eigenspaces, consistent with the real inertia calculation.
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