Trying to interpret matrix representations of operators

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SUMMARY

The discussion centers on the interpretation of matrix representations of operators, specifically a 3x3 operator Q, and its eigenvectors and eigenvalues. The participant confirms that the eigenvectors correspond to eigenfunctions, and when measuring the state represented by a 3x1 matrix [b], it can be expressed as a linear combination of these eigenvectors. The analogy to Schrödinger's cat is drawn, illustrating that prior to measurement, the state is a superposition, and upon measurement, the system collapses into one of the eigenstates of Q, confirming the probabilistic nature of quantum mechanics.

PREREQUISITES
  • Understanding of linear algebra concepts, particularly eigenvectors and eigenvalues.
  • Familiarity with quantum mechanics principles, especially wavefunction collapse.
  • Knowledge of matrix representations of operators in quantum systems.
  • Basic comprehension of superposition in quantum states.
NEXT STEPS
  • Study the mathematical formulation of quantum mechanics, focusing on operators and their eigenstates.
  • Learn about the implications of measurement in quantum mechanics, particularly the collapse of the wavefunction.
  • Explore the relationship between linear combinations of eigenvectors and physical states in quantum systems.
  • Investigate further into the concept of superposition and its applications in quantum computing.
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Quantum physicists, students of quantum mechanics, and anyone interested in the mathematical foundations of quantum theory and operator theory.

nabeel17
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Say I have a 3x3 operator Q and I find its eigenvectors and eigenvalues. Now i know that those eigenvectors are the same as eigenfunctions so if i act on them with Q i will get the corresponding eigenvalue.

What the question I am trying to solve asks is, Measure the quantity Q in state where b is given as a 3x1 matrix. I know how to do it mathematically, I just express as a linear combination of my eigenvectors. But I'm trying to interpret what this means. Is the state some state my wavefunction is in and when I measure it, it will be in a state of one of the eigenvectors of Q?

I am comparing this to Schrodingers cat where before I measure it is in a linear combination of alive and dead and there is a probability that can be alive or dead and when I measure (ie look) the wavefunction collapses to either alive or dead. Am i correct in thinking this way about Q and ?
 
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yeah, that's right. When they say a measurement of the physical quantity associated with Q, that means the state suddenly jumps into one of the eigenstates of Q.
 
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