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    No non-zero operator on $\CC^2$ is everywhere imaginary-orthogonal

    E-HK-81-7

    Area
    Algebra
    Topics
    Inner Product Spaces, Linear Algebra, Linear Transformations
    Status
    draft

    Let \(( \mid )\) be the standard inner product on \(C^2\). Prove that there is no non-zero linear operator on \(C^2\) such that \((\alpha \mid T\alpha) = 0\) for every \(\alpha\) in \(C^2\). Generalize.

    Solution

    1. The Complex Polarization Identity:

    1.1. Let \(V\) be an inner product space over the complex field \(\mathbb{C}\) with inner product \((\cdot \mid \cdot)\), and let \(T: V \to V\) be a linear operator.

    setup.

    1.2. For any \(\alpha, \beta \in V\) and each \(k \in \{0, 1, 2, 3\}\), expand the quadratic form at \(\alpha + i^k \beta\):\[ \big(\alpha + i^k \beta \mid T(\alpha + i^k \beta)\big) = (\alpha \mid T\alpha) + i^k (\alpha \mid T\beta) + \overline{i^k} (\beta \mid T\alpha) + (\beta \mid T\beta). \]

    conjugate-linearity in the first argument and linearity in the second argument.

    1.3. Multiply by \(i^k\) and sum over \(k \in \{0, 1, 2, 3\}\):- \(\sum_{k=0}^3 i^k = 1 + i - 1 - i = 0\),- \(\sum_{k=0}^3 i^{2k} = 1 - 1 + 1 - 1 = 0\),- \(\sum_{k=0}^3 i^k \overline{i^k} = \sum_{k=0}^3 |i^k|^2 = 4\).Thus:\[ \sum_{k=0}^3 i^k \big(\alpha + i^k \beta \mid T(\alpha + i^k \beta)\big) = 4 (\alpha \mid T\beta). \]

    sum of powers of \(i\).

    2. Proof that \((v \mid Tv) = 0\) for all \(v\) forces \(T = 0\):

    2.1. By hypothesis, \((v \mid Tv) = 0\) for all \(v \in V\).Applying this to the four vectors \(v_k = \alpha + i^k \beta\) gives:\[ (\alpha \mid T\beta) = \frac{1}{4} \sum_{k=0}^3 i^k (v_k \mid T v_k) = \frac{1}{4} \sum_{k=0}^3 i^k \cdot 0 = 0 \quad \text{for all } \alpha, \beta \in V. \]

    polarization identity from 1.

    2.2. For each \(\beta \in V\), choose \(\alpha = T\beta\):\[ \|T\beta\|^2 = (T\beta \mid T\beta) = 0 \implies T\beta = 0. \]

    positive definiteness of inner products.

    2.3. Since \(T\beta = 0\) for every \(\beta \in V\), \(T\) is the zero operator (\(T = 0\)).

    definition of the zero operator.

    3. Generalization and Comparison with Real Spaces:

    3.1. Generalization: The result holds for any complex inner product space \(V\) (of arbitrary dimension):If \((v \mid Tv) = 0\) for all \(v \in V\), then \(T = 0\).

    polarization holds over any complex inner product space.

    3.2. Real vs Complex Distinction: Over a real inner product space, this property fails:For example, on \(\mathbb{R}^2\) with standard inner product, the \(90^\circ\) rotation \(T(x, y) = (-y, x)\) satisfies \((v \mid Tv) = -xy + yx = 0\) for all \(v \in \mathbb{R}^2\), yet \(T \neq 0\).

    skew-symmetric operators over \(\mathbb{R}\).

    4. Conclusion:There is no non-zero linear operator on \(\mathbb{C}^2\) (or any complex inner product space) such that \((\alpha \mid T\alpha) = 0\) for all \(\alpha\). Q.E.D.

    1 through 3.