What is the significance of matrix elements of vectors in quantum mechanics?

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SUMMARY

The discussion focuses on the significance of matrix elements of vectors in quantum mechanics, specifically in the context of operators and states. In quantum mechanics, a state is represented as a vector, and an operator is represented as a matrix when a basis is chosen. The matrix elements are defined by their positions in the matrix, such as the Pauli matrices representing spin operators. The examples provided illustrate how to compute specific matrix elements using the Pauli matrix σz.

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  • Knowledge of Pauli matrices and their role in quantum mechanics.
  • Basic proficiency in vector notation and operations.
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What exactly is all this 'matrix elements of vectors' stuff that Landau is talking about?

I don't mean to ask people unfamiliar with this section to read it for me, so hopefully for someone who's read it - what's going on and where would I find a more modern discussion of this section (I'm sure this whole chapter should become easy when written in modern notation)?

Thanks!
 
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A state in quantum mechanics is a vector. If one chooses a basis, it has a representation as a column vector.

An operator in quantum mechanics is a linear operators on the state, so again, if one chooses a basis, the operator has a representation as a matrix. The matrix elements are labelled according to the row and column of the matrix.

Here is an example. The Pauli matrices are a representation of the spin operators, written in the basis such the a spin in the +z direction is the column vector [1 0]T, and a spin in the -z direction is the column vector [0 1]T.
http://faculty.cua.edu/sober/611/Spin_and_Pauli_matrices.pdf
http://web.uconn.edu/~ch351vc/pdfs/spin1.pdf

To get the matrix element that is in the first row and first column of the σz Pauli matrix, one does:
<spin in up direction|σz|spin in up diection> = [1 0]σz[1 0]T

To get the matrix element that is in the second row and first column of the σz Pauli matrix, one does:
<spin in down direction|σz|spin in up diection> = [0 1]σz[1 0]T
 
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