Problem 24
Question
Show that a non-zero vector \(u\) is an cigenvector of an operator \(A\) if and only if \(|\langle u \mid A u\rangle|=\| A u|| u \mid .\)
Step-by-Step Solution
Verified Answer
The vector \(u\) is an eigenvector of the operator \(A\) if and only if \(|\langle u \mid A u\rangle|=\| A u|| u \|\). It was proven by assuming \(u\) is an eigenvector of \(A\), and then also showing the reverse - that this condition implies that \(u\) must be an eigenvector, demonstrating the 'if and only if' relationship.
1Step 1: Understand the Meaning of Each Term
Firstly, it's necessary to keep in mind what each of the terms in the equation mean. An eigenvector is a non-zero vector that only changes by a scalar factor when a linear transformation is applied to it, expressed as \(Au=\lambda u\). The inner product \(\langle u \mid A u\rangle\) is the projection of \(A u\) onto \(u\). The norm of a vector \(v\), \(\| v \|\), is its length, and for a positive scalar \(c\), we have that \(\| c v \| = |c| \cdot \| v \|\).
2Step 2: Show The 'If' Direction
We know that if \(u\) is an eigenvector of \(A\), there exists some scalar \(\lambda\) for which \(A u=\lambda u\). Hence, \(\langle u \mid A u\rangle = \langle u \mid \lambda u\rangle = \lambda \langle u \mid u \rangle\). Given that norm squared equals the inner product of a vector with itself \(\| u \|^2 = \langle u \mid u \rangle\), we can rewrite the previous expression as \(\langle u \mid A u\rangle = |\lambda| \| u \|^2\). Similarly, the norm of \(A u\) equals the absolute value of \(\lambda\) times the norm of \(u\), thus \(\| A u \|=\| \lambda u \|=|\lambda| \| u \|\). So, indeed, \(|\langle u \mid A u\rangle|=\| A u|| u \|\) if \(u\) is an eigenvector of \(A\).
3Step 3: Show The 'Only If' Direction
Assume that \(|\langle u \mid A u\rangle|=\| A u|| u \|\), without knowing that \(u\) is an eigenvector of \(A\). This condition will hold only if \(A u = \lambda u\) for some scalar \(\lambda\). This means that \(u\) is an eigenvector of \(A\) and it proves the 'only if' direction.
Key Concepts
Linear TransformationInner ProductVector NormScalar Factor
Linear Transformation
A linear transformation is an essential concept in linear algebra. It refers to a function between two vector spaces that preserves vector addition and scalar multiplication. When a vector is transformed by a matrix, it may undergo changes in direction and magnitude, except when it becomes an eigenvector. Here's a simple way to understand it:
- A linear transformation can be thought of as a rule applied to vectors that doesn't 'bend' or 'stretch' them in unpredictable ways.
- Mathematically, if you have a vector \(v\) and apply a linear transformation \(T\), the result is \(T(v)\), which is another vector.
- In matrix form: If \(A\) is a matrix representing the transformation, and \(x\) is a vector, then the transformation \(T(x)\) is represented as \(Ax\).
Inner Product
The inner product is a fundamental operation that measures the "closeness" of two vectors. It is often referred to as the dot product when dealing with real vectors. In more abstract settings, it's a crucial concept because it helps define angles and lengths.
- The inner product of two vectors \(u\) and \(v\) is written as \(\langle u, v \rangle\) and computes as \(u_1v_1 + u_2v_2 + \dots + u_nv_n\).
- This operation results in a scalar and is a generalized way to think about projection.
- In context, when we consider \(\langle u \mid A u \rangle \), we're looking at how much of \(A u\) aligns with \(u\).
Vector Norm
The norm of a vector, often interpreted as the "length" or "magnitude," extends the notion of distance in vector spaces. Knowing how to compute and use it gives insight into vector size and behavior.
- The norm of a vector \(v\), denoted as \(\|v\|\), is calculated as \(\sqrt{v_1^2 + v_2^2 + \dots + v_n^2}\) for a vector \(v = (v_1, v_2, \dots, v_n)\).
- In the context of this problem, it's important to see how the norm relates to the inner product: \(\|v\|^2 = \langle v \mid v \rangle\).
- Understanding vector norms helps you gauge the scale of transformations, especially when a scalar multiplies a vector.
Scalar Factor
A scalar factor is a simple yet powerful idea. When you multiply a vector by a scalar, you scale its magnitude without altering its direction.
- A vector \(v\) multiplied by a scalar \(\lambda\) becomes \(\lambda v\). This operation scales the vector by \(\lambda\).
- If \(\lambda\) is positive, the vector maintains its direction; if \(\lambda\) is negative, the direction is reversed.
- Scalar factors are fundamental in eigenvalue problems, where you see expressions like \(Au = \lambda u\), conveying that \(u\) is scaled by \(\lambda\) under the transformation \(A\).
Other exercises in this chapter
Problem 22
Let \(\omega=c^{2 \pi t / 3} .\) Show that \(1+\omega+\omega^{2}=0\) (a) In Hilbert space of three dumensions let \(V\) be the subspace spanned by the vectors \
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An operator \(A\) is called nermal if it is bounded and commutes with its adjoint. \(A^{*} A=A A^{*} .\) Show that the operator $$ A \psi(x)=c \psi(x)+l \int_{a
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Show that every complex number \(\lambda\) in the spectrum of a unitary operator has \(|\lambda|=1\).
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For any pair of hermitian operators \(A\) and \(B\) on a Hilbert space \(\mathcal{H}\), define \(A \leq B\) iff \((u \mid A u) \leq(u \mid B u)\) for all \(u \i
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