Are Both Eigenvectors Correct?

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SUMMARY

Both eigenvectors derived from an eigenvalue are valid, as scalar multiplication of an eigenvector results in another eigenvector. For instance, the eigenvector \(\begin{bmatrix} 1 \\ \frac{1}{3} \end{bmatrix}\) is equivalent to \(\begin{bmatrix} 3 \\ 1 \end{bmatrix}\) when multiplied by the scalar 3. This principle is grounded in the definition of eigenvectors, confirming that multiple representations of the same eigenvector are acceptable.

PREREQUISITES
  • Understanding of eigenvalues and eigenvectors
  • Familiarity with linear algebra concepts
  • Knowledge of scalar multiplication in vector spaces
  • Basic proficiency in matrix representation
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  • Study the properties of eigenvectors and eigenvalues in linear algebra
  • Explore scalar multiplication and its implications in vector spaces
  • Learn about the geometric interpretation of eigenvectors
  • Investigate applications of eigenvectors in data science and machine learning
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Students and professionals in mathematics, particularly those studying linear algebra, as well as data scientists and engineers applying eigenvector concepts in computational algorithms.

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say for example when I calculate an eigenvector for a particular eigenvalue and get something like
\begin{bmatrix}<br /> 1\\<br /> \frac{1}{3}<br /> \end{bmatrix}

but the answers on the book are

\begin{bmatrix}<br /> 3\\<br /> 1<br /> \end{bmatrix}

Would my answers still be considered correct?
 
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Yes, multiplying an eigenvector with a scalar yields another eigenvector (makes kind of sense right? Think about the definition). Usually people will multiply the result with whatever scalar makes all the entries integers for representation purposes, but both results are correct.
 
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I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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