Are state vectors and wavefunctions the same?

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Discussion Overview

The discussion centers on the relationship between state vectors (kets) and wavefunctions in the context of quantum mechanics, specifically regarding their existence in Hilbert space and their mathematical representations. Participants explore theoretical implications, definitions, and interpretations related to these concepts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants assert that state vectors live in Hilbert space, questioning whether wavefunctions also inhabit this space and how functions and vectors can coexist within it.
  • Others propose that any collection of elements can form a vector space if the axioms are satisfied, suggesting that wavefunctions can be considered vectors in this context.
  • A participant references a Wikipedia entry to clarify that wavefunctions are projections of state vectors onto a position basis, indicating a distinction between the two concepts.
  • It is noted that mathematicians may prefer to use wavefunctions rather than state vectors, as the latter may lack meaning without a specific representation.
  • Some argue that functions and vectors are isomorphic, allowing them to be treated similarly mathematically, with examples like orthogonal bases provided.
  • Another participant highlights that Dirac notation is basis-independent, while wavefunctions imply a chosen basis, which could affect their interpretation.
  • A later reply discusses the role of wavefunctions in describing pure states in the Schrödinger representation, contrasting this with the definition of state vectors in Hilbert space.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between state vectors and wavefunctions, with no consensus reached on whether they are equivalent or how they should be defined within the framework of quantum mechanics.

Contextual Notes

Limitations in definitions and interpretations are evident, as participants navigate the nuances of mathematical representations and the implications of different bases in quantum mechanics.

emob2p
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Hi,
State vectors ("kets") live in Hilbert space. Do wavefunctions also live in Hilbert space? I've read that they both do, but how can functions and vectors reside in the same space? Or do wave functions simply map from coordinate space to Hilbert space?
Thanks
 
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Any collection of things can form a vector space, as long as the axioms of a vector space are satisfied.
 
Hello emob2p,

I just found in wikipedia
http://en.wikipedia.org/wiki/Wave_mechanics#The_wavefunction

"We define the wavefunction as the projection of the state vector |ψ(t)> onto the position basis:
[tex]\Psi(r,t) = \langle r|t \rangle[/tex]"

I think the difference, as mentioned above, is that a state vector (in Dirac representation) looks like this: |Psi> , |a> , |b> ..., it has so to say no representation, only this strange "|blabla>" one. This |Psi> contains all the information you can have about a physical system.

But when you talk of a wavefunction, you have a certain representation, for example: space, then you have [tex]\Psi (x) = \langle x|\Psi (x) \rangle[/tex], or in momentum representation, you have [tex]\Psi (p) = \langle p|\Psi (x) \rangle[/tex].

Mathematicians don't like the Dirac notation ([tex]|\Psi \rangle[/tex]), if I remember correctly. They only have the wavefunctions ([tex]\Psi (x)[/tex], but not the state vectors alone.
For them, the state vector alone makes no sense (correct me if I'm wrong), so they don't use this term "state vector".

A second interpretation could be that mathematicians do use the term "state vectors" for the wavefunctions. The reason would be that wavefunctions are elements of a vector space, and mathematicians call all the elements of V vectors.

Maybe a mathematician could tell you more about this and the rigorous definitions.
 
Last edited:
Maybe a mathematician could tell you more about this and the rigorous definitions.
Any collection of things can form a vector space, as long as the axioms of a vector space are satisfied. :biggrin:

You can form a Hilbert space from the set of all square-integrable functions on the real line. When working with that Hilbert space, you would call a square-integrable function of the real line a vector. If you take that Hilbert space to be your state space, then you would call a square-integrable function of the real line a state vector.
 
emob2p said:
Hi,
State vectors ("kets") live in Hilbert space. Do wavefunctions also live in Hilbert space? I've read that they both do, but how can functions and vectors reside in the same space? Or do wave functions simply map from coordinate space to Hilbert space?
Thanks


wrt vectors and functions both reside in the same space its important to know that functions and vectors are isomorphic, that is, can be treated the same mathematically. The set of polynomials all form an orthogonal basis, that is x is orthogonal to [tex]x^2[/tex] which is orthogonal to [tex]x^3[/tex] etc... (there is some normalization coeficients I've missed off but you get the picture). You can look this up more - Gram Schmidt Orthogonalization and I think Legendre Polynomials.
 
The key benefit of Dirac notation is that it is basis independent, which makes it more general in a sense. By writing down a wave function you have implicitly chosen a basis (the position representation, in most textbooks).
 
There's something simple here. Or at least it seems simple. The "wavefunction" is a term one uses to name the mathematical objects (either functions,functionals or vectors, "objects" in general) which fully describe pure states in the Schrödinger representation (so-called "wave mechanics") of the Born-Jordan CCR. While "state vector" is the vector in the Hilbert space (or the linear functional continuous on the nuclear subspace associated to an unbounded selfadjoint densly defined linear operator) which "pinpoints" the (unit) ray which describes the pure quantum state in the fundamental formulation on (nonrelativistic) quantum mechanics.

Daniel.
 

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