Representing |psi> with Continuous Eigenvectors: An Example

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SUMMARY

The discussion focuses on representing the quantum state vector |psi> using continuous eigenvectors, specifically in the context of position eigenvectors {|x>}. The state vector is expressed as |\psi\rangle = C_n |x\rangle, where C_n = . The spectral value of the operator X is clarified as synonymous with the eigenvalue, providing a foundational understanding of how continuous eigenvalues relate to state representation in quantum mechanics.

PREREQUISITES
  • Understanding of quantum mechanics, specifically state vectors and eigenvalues.
  • Familiarity with Dirac notation, including kets and bras.
  • Knowledge of continuous eigenvalue problems in quantum systems.
  • Basic concepts from Griffiths' "Introduction to Quantum Mechanics," particularly Chapter 3.
NEXT STEPS
  • Study the representation of state vectors in quantum mechanics using continuous eigenvalues.
  • Learn about the mathematical formulation of position operators and their eigenstates.
  • Explore the implications of spectral values in quantum mechanics.
  • Review examples of continuous basis vectors in quantum systems beyond position eigenvectors.
USEFUL FOR

Students of quantum mechanics, physicists working with continuous eigenvalue problems, and anyone seeking to deepen their understanding of state vector representation in quantum systems.

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Homework Statement


for discrete basis vectors {{e_n}}, a state vector |psi> is represented by a column vector, with elements being psi_n = <e_n|psi>. When basis vectors correspond to those with continuous eigenvalues, vectors are represented by functions. Give such an example of a state vector |psi> being represented in a space spanned by position eigenvectors {|x>}.


Homework Equations




The Attempt at a Solution



C_n = <x_n | psi>

I'm really taking a shot in the dark with this one. I'm using Griffith's, so I assume my solutions lies somewhere in chapter 3.
 
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So...|\psi\rangle is a ket which is part of the space spanned by eigenvectors of X, the latter being kets satisfying X|x\rangle = x |x\rangle, where the x is a real number, the spectral value of X.

Soo... |\psi\rangle = \mbox{(something)} ~ |x\rangle

What's (something) equal to ?
 


When you say spectral value, is that the same as the eigenvalue?
 


A generalization of eigenvalue. But you can think of it in a simplified way as an eigenvalue.
 

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