Where to learn the matrix formulation of QM

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Discussion Overview

The discussion centers on resources for learning the matrix formulation of quantum mechanics (QM), specifically how to represent the Hamiltonian as a matrix. Participants seek guidance on materials that focus on this approach rather than the calculus-based methods that are more commonly available.

Discussion Character

  • Exploratory, Technical explanation, Homework-related

Main Points Raised

  • One participant expresses difficulty in finding resources specifically focused on the matrix formulation of QM and requests links for learning.
  • Another participant suggests a Wikipedia page on bra-ket notation as a starting point for understanding the matrix formulation.
  • A third participant provides a link to a lecture series and mentions the Feynman lectures, explaining that in a given basis, vectors can be represented as column vectors and discusses the differences between finite and infinite dimensional vector spaces.
  • This same participant also points out that operators can be represented as matrices when considering states as column vectors in a certain basis and provides a link to a tutorial on effective Hamiltonians as a practical example.
  • Another participant recommends the book "Quantum Mechanics" by Claude Cohen-Tannoudji as a helpful resource.

Areas of Agreement / Disagreement

Participants do not appear to reach a consensus on a single resource but offer various suggestions and perspectives on where to find information about the matrix formulation of QM.

Contextual Notes

The discussion reflects a range of resources and approaches, but it does not resolve the best method for learning the matrix formulation, nor does it clarify the completeness or suitability of the suggested materials.

Superposed_Cat
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Hi, material on learning the calculus way are plentiful but I can't find anywhere to teach me the matrix way, any links? I can't even find out how to represent the Hamiltonian as a matrix. Thanks in advance
 
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http://www.theory.caltech.edu/people/preskill/ph229/#lecture (Chapter 2)

Take a look also at the third volume of the Feynman lectures.

In a given basis, a vector has a representation as a column vector vi, where i is a discrete index. The number of indices is the dimension of the vector space. You can think of the position space wavefunction ψ(x) similarly as the representation of a vector in the position basis, except that the index x is continuous. Since there are now an infinite number of indices, the dimension of the vector space is infinite. There are differences between finite and infinite dimensional vector spaces, but using the finite dimensional case for intuition is roughly ok. Now sticking to the finite dimensional case, if we think of the state as a column vector in a certain basis, an operator on the state can be represented as a matrix.

For an example of the practical use of the Hamiltonian as a matrix try http://condensedconcepts.blogspot.sg/2013/10/tutorial-on-effective-hamiltonians-for.html
 
Last edited:
I found most helpful the Quantum Mechanics by Claude Cohen-Tannoudji
 

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