What is an Eigenstate in Relation to Schrodinger Equation?

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Discussion Overview

The discussion centers around the concept of eigenstates in relation to the Schrödinger equation, exploring their definitions, properties, and connections to linear operators in quantum mechanics. Participants examine the nature of eigenstates, their role as solutions to equations, and the implications of different types of operators.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants assert that eigenstates are directly related to the Schrödinger equation and can be expressed as a linear sum of eigenstates of a linear operator.
  • Others clarify that eigenstates are solutions to the eigenvalue problem of an operator corresponding to an observable, with energy eigenstates specifically being solutions to the time-independent Schrödinger equation.
  • A distinction is made between eigenstates of different operators, such as the Hamiltonian and raising/lowering operators, with some arguing that not all operators have eigenstates.
  • There is a discussion about the nature of solutions, with some participants emphasizing that eigenstates are defined without reference to the Schrödinger equation.
  • Participants debate the implications of operators being Hermitian, with some stating that only Hermitian operators have a complete set of eigenstates, while others argue that non-Hermitian operators can still have eigenstates.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between eigenstates and the Schrödinger equation, the nature of solutions, and the properties of various operators. The discussion remains unresolved with multiple competing perspectives on these topics.

Contextual Notes

There are unresolved nuances regarding the definitions and properties of eigenstates, particularly in relation to different types of operators and the conditions under which they possess eigenstates.

CookieSalesman
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What is an eigenstate in relation to the Schrödinger equation?

We've been working with this stuff but I don't exactly understand what that is.
I know of linear algebra eigenstates or eigenfunctions but I don't know if they are directly related.
 
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They are directly related. The set of all eigenstates of a non-degenerate linear operator form a basis for the vector space, which in the Schrödinger case is the vector space of all possible configurations of the system.

In the Schrödinger equation, we can use this basis property to express the initial state as a linear sum of eigenstates of a particular linear operator. The Schrödinger equation then tells us that each of those evolves over time by the scalar multiplier ##e^{ikt}## changing with time ##t##. The scalar multiplier is the 'phase'. Because ##k## differs between different eigenstates, the periods for phase variation vary between eigenstates, so the relative phase changes, which means that the overall state, which is the sum of the individual components, varies over time in a way that is not just a scalar multiplier.
 
CookieSalesman said:
What is an eigenstate in relation to the Schrödinger equation?
If you're working with the Schrödinger equation, you're probably working with wavefunctions ##\psi(x,t)## or ##\psi(x)##.

If ##\psi## is an eigenstate of an operator, then when you apply the operator to ##\psi##, you get ##\psi## multiplied by a constant (the eigenvalue).

For example, if ##\psi## is an eigenstate of the momentum operator ##-i\hbar \frac {\partial} {\partial x}##, then $$-i\hbar \frac {\partial \psi} {\partial x} = p\psi$$ where ##p## is the eigenvalue, i.e. the momentum of that state.
 
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thx guys
 
So more or less, eigenstates are simply solutions?
 
CookieSalesman said:
So more or less, eigenstates are simply solutions?
Yes. They are solutions to the eigenvalue-problem of the operator corresponding to the observable in question.
 
CookieSalesman said:
So more or less, eigenstates are simply solutions?

Not really. Energy Eigenstates are solutions to the time independent Schrödinger equation, each for a corresponding energy value.

But, more generally, any linear operator has its eigenstates. It is an assumption in QM that any operator that represents an observable has a complete set of orthogonal eigenstates. The Hamiltonian being a specific example of this.

Other operators may have eigenstates with different properties. The raising and lowering operators of the harmonic oscillator are good examples. The eigenstates of the lowering operator are the so-called coherent states. And the raising operator has no eigenstates.

PS eigenstates relate directly to linear operators are are really only indirectly related the Schrödinger equation itself.
 
Last edited:
PeroK said:
Not really. Energy Eigenstates are solutions to the time independent Schrödinger equation, each for a corresponding energy value.

But, more generally, any linear operator has its eigenstates. It is an assumption in QM that any operator that represents an observable has a complete set of orthogonal eigenstates. The Hamiltonian being a specific example of this.

Other operators may have eigenstates with different properties. The raising and lowering operators of the harmonic oscillator are good examples. The eigenstates of the lowering operator are the so-called coherent states. And the raising operator has no eigenstates.

PS eigenstates relate directly to linear operators are are really only indirectly related the Schrödinger equation itself.
Ok but it seems like you just said eigenstates are solutions. YOu said that any linear operator has its eigenstates so those eigenstates are simply "solutions" corresponding to specific quantum numbers right?
 
CookieSalesman said:
Ok but it seems like you just said eigenstates are solutions. YOu said that any linear operator has its eigenstates so those eigenstates are simply "solutions" corresponding to specific quantum numbers right?

Nothing is a "solution". Things are solutions to specific equations.

Energy eigenstates are solutions to the time independent Schrödinger equation.

Energy eigenstates are not solutions to the full Schrödinger equation. For that you need to include a function of time, related to the energy.

An eigenstate of a linear operator is well defined without any reference whatsoever to the Schrödinger equation or to QM for that matter. It is defined as a solution to the eigenvalue equation for that operator.
 
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  • #10
PeroK said:
Energy eigenstates are solutions to the time independent Schrödinger equation.
To make this more explicit, the operator in question here is the Hamiltonian operator: $$\hat H = -\frac {\hbar^2} {2m} \frac {\partial^2} { \partial x^2} + V(x)$$ Written in the form of an eigenvalue equation, the Schrödinger equation is ##\hat H \psi = E \psi##.
 
  • #11
PeroK said:
[...] But, more generally, any linear operator has its eigenstates. [...] And the raising operator has no eigenstates.[...]

This is a self-contradiction. Can you, please, re-phrase your opinion?
 
  • #12
dextercioby said:
This is a self-contradiction. Can you, please, re-phrase your opinion?
I think the sentence just inadvertently lacks the word 'Hermitian'. Any Hermitian operator has a complete basis of eigenstates. The raising operator is not Hermitian.
 
  • #13
dextercioby said:
This is a self-contradiction. Can you, please, re-phrase your opinion?

Any linear operator has a set of eigenstates. That set may be empty.
 
  • #14
andrewkirk said:
I think the sentence just inadvertently lacks the word 'Hermitian'. Any Hermitian operator has a complete basis of eigenstates. The raising operator is not Hermitian.

Yes, the raising operator is not Hermitean, but this doesn't mean it has no eigenstates.
 
  • #15
dextercioby said:
Yes, the raising operator is not Hermitean, but this doesn't mean it has no eigenstates.
Sure, I didn't say it did. But with the insertion of 'Hermitian' in the post, it is not self-contradictory, which is what was being discussed.
 
  • #16
Alright, putting "hermitean" there is a step forward as the first statement is rephrased. The raising operator has eigenstates, it's then the second statement of the two I quoted that is wrong.
 

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