Why the linear combination of eigenfunctions is not a solution of the TISE

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Discussion Overview

The discussion revolves around the relationship between the time-dependent Schrödinger equation (TDSE) and the time-independent Schrödinger equation (TISE), particularly focusing on the conditions under which eigenfunctions can be considered solutions to the TISE. Participants explore the implications of a time-independent Hamiltonian on the applicability of these equations, raising questions about the nature of solutions and the concept of stationary states.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants assert that the linear combination of eigenfunctions should provide a solution to the TISE, but note that this is not always true when eigenvalues are not equal.
  • Others clarify that the TDSE remains time-dependent even when the Hamiltonian is time-independent due to the presence of the time derivative term.
  • Several participants emphasize that the TISE and TDSE are distinct equations, with the TISE describing stationary states and the TDSE governing the time evolution of the system.
  • There is a discussion about the significance of the Hamiltonian being time-independent, with some suggesting that it does not imply that the system can be described solely by the TISE.
  • Some participants express confusion regarding when to use the TISE versus the TDSE, questioning the properties required for each equation's applicability.
  • It is noted that while the TISE provides a basis for stationary states, the TDSE is necessary for computing time evolution in both time-independent and time-dependent Hamiltonian scenarios.

Areas of Agreement / Disagreement

Participants generally do not reach a consensus, as there are multiple competing views regarding the relationship between the TISE and TDSE, particularly in the context of time-independent Hamiltonians. Confusion persists about the conditions under which each equation should be applied.

Contextual Notes

Some participants highlight that the eigenfunctions of the Hamiltonian, while useful for expressing general states, do not necessarily serve as solutions to the TISE in all cases, particularly when considering the implications of time dependence.

Physicslad00
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TL;DR
The linear combination of the eigenfunctions gives solution to the Schrodinger equation. For a system with time independent Hamiltonian the Schrodinger Equation reduces to the Time independent Schrodinger equation(TISE), so this linear combination should be a solution of the TISE. It is not always true(when eigenvalues are not equal). Why is it so?
The linear combination of the eigenfunctions gives solution to the Schrödinger equation. For a system with time independent Hamiltonian the Schrödinger Equation reduces to the Time independent Schrödinger equation(TISE), so this linear combination should be a solution of the TISE. It is not always true(when eigenvalues are not equal). Why is it so?

Please tell me where am I going wrong.
 
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The Schroedinger equation is ##i\hbar \partial_t \Psi(t,\vec x) = (\hat H(t) \Psi)(t,\vec x)##. If ##\hat H(t) = \hat H## is time-independent, the equation is still time-dependent through ##\partial_t##. An eigenfunction of ##\hat H## satisfies the time-independen Schroedinger equation ##(\hat H \psi)(\vec x) = E \psi(\vec x)## and doesn't depend on ##t##. So if we insert it into the time-dependent Schroedinger equation, we get ##i\hbar\partial_t \psi(\vec x) = 0 = (\hat H \psi)(\vec x) = E\psi(\vec x)##, which is false, because ##\psi(\vec x)\neq 0##.

If you have a solution ##\psi(\vec x)## to the time-independen Schroedinger equation ##(\hat H \psi)(\vec x) = E\psi(\vec x)##, you can turn it into a solution of the time-dependen Schroedinger equation by multiplying it by a phase factor: ##\Psi(t,\vec x) = e^{-\frac{i}{\hbar} E t}\psi(\vec x)##
 
Nullstein said:
The Schroedinger equation is ##i\hbar \partial_t \Psi(t,\vec x) = (\hat H(t) \Psi)(t,\vec x)##. If ##\hat H(t) = \hat H## is time-independent, the equation is still time-dependent through ##\partial_t##. An eigenfunction of ##\hat H## satisfies the time-independen Schroedinger equation ##(\hat H \psi)(\vec x) = E \psi(\vec x)## and doesn't depend on ##t##. So if we insert it into the time-dependent Schroedinger equation, we get ##i\hbar\partial_t \psi(\vec x) = 0 = (\hat H \psi)(\vec x) = E\psi(\vec x)##, which is false, because ##\psi(\vec x)\neq 0##.

If you have a solution ##\psi(\vec x)## to the time-independen Schroedinger equation ##(\hat H \psi)(\vec x) = E\psi(\vec x)##, you can turn it into a solution of the time-dependen Schroedinger equation by multiplying it by a phase factor: ##\Psi(t,\vec x) = e^{-\frac{i}{\hbar} E t}\psi(\vec x)##
I don't understand why the SE is time dependent even when the hamiltonian is time independent?
 
Physicslad00 said:
For a system with time independent Hamiltonian the Schrödinger Equation reduces to the Time independent Schrödinger equation(TISE)
No, it doesn't. They are still two different equations.

The time-dependent Schrödinger Equation for a time-independent Hamiltonian is

$$
i \hbar \frac{\partial \psi}{\partial t} = \hat{H} \psi
$$

The TISE is

$$
\hat{H} \psi = E \psi
$$

These equations are not the same.
 
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Physicslad00 said:
I don't understand why the SE is time dependent even when the hamiltonian is time independent?
Because it has ##\partial_t \psi## on the LHS. That is time dependence.
 
Physicslad00 said:
I don't understand why the SE is time dependent even when the hamiltonian is time independent?
It's an evolution equation. Given an initial state ##\Psi(0,\vec x)##, you want to evolve it to a state ##\Psi(t,\vec x)##, so naturally, there must be a time-dependence somewhere. In the TDSE, it's in the ##\partial_t## time derivative. As an analogy, Newton's equations of motion are also time-dependent, even if the force isn't.
 
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PeterDonis said:
No, it doesn't. They are still two different equations.

The time-dependent Schrödinger Equation for a time-independent Hamiltonian is

$$
i \hbar \frac{\partial \psi}{\partial t} = \hat{H} \psi
$$

The TISE is

$$
\hat{H} \psi = E \psi
$$

These equations are not the same.
Does this mean that Hamiltonian being time independent does not imply that the system is described by TISE. I have confusion regarding when to use TISE and TDSE for a system. All this while i had thought that if a system has time independent Hamiltonian then it should be described by TISE, but your comment makes me think that this is wrong. Can you please tell how and when do we use TISE and TDSE, and what should be the properties of the system to use either of them. Thanks
 
Physicslad00 said:
I have confusion regarding when to use TISE and TDSE for a system.
The TDSE is what "describes" the system in general, in the sense that any possible state of the system will be a solution of the TDSE.

The TISE is used to figure out what the "stationary states" of the system are. Strictly speaking, these states are not actually "stationary"--they still do change with time. But the change with time is a pure phase factor, as @Nullstein said. That means that no observables change with time, since a pure phase factor has no effect on any observables. One can think of the solutions of the TISE as describing the stationary states of the system at time ##t = 0##, when the phase factor ##e^{i E t}## is just ##1##.

The reason knowing the stationary states is useful is that they provide a convenient basis in which to express general states; that is, any state of the system (that is, any solution of the TDSE) can be expressed as a linear combination of one or more stationary states.
 
PeterDonis said:
The TDSE is what "describes" the system in general, in the sense that any possible state of the system will be a solution of the TDSE.

The TISE is used to figure out what the "stationary states" of the system are. Strictly speaking, these states are not actually "stationary"--they still do change with time. But the change with time is a pure phase factor, as @Nullstein said. That means that no observables change with time, since a pure phase factor has no effect on any observables. One can think of the solutions of the TISE as describing the stationary states of the system at time ##t = 0##, when the phase factor ##e^{i E t}## is just ##1##.

The reason knowing the stationary states is useful is that they provide a convenient basis in which to express general states; that is, any state of the system (that is, any solution of the TDSE) can be expressed as a linear combination of one or more stationary states.
When the Hamiltonian is time independent, can't we use the TISE to describe the system in general?
 
  • #10
Physicslad00 said:
Does this mean that Hamiltonian being time independent does not imply that the system is described by TISE. I have confusion regarding when to use TISE and TDSE for a system. All this while i had thought that if a system has time independent Hamiltonian then it should be described by TISE, but your comment makes me think that this is wrong. Can you please tell how and when do we use TISE and TDSE, and what should be the properties of the system to use either of them. Thanks
You always use the TDSE if you want to compute the time evolution. The TISE is not so much a physical equation, but rather a convenient tool for intermediate calculations, because knowing the eigenfunctions is quite helpful. (However, it still has physical content. The eigenvalues are relevant in measurement theory.)
 
  • #11
Physicslad00 said:
When the Hamiltonian is time independent, can't we use the TISE to describe the system in general?
Go read my post again. It answers this question. In particular, read the last sentence of the second paragraph.
 
  • #12
PeterDonis said:
Go read my post again. It answers this question. In particular, read the last sentence of the second paragraph.
I understand that the eigenfunctions act as basis to describe the wavefunctions which are general solution of TDSE. What I can't understand is the significance of Hamiltonian being time independent. When the Hamiltonian is time dependent, we use TDSE to describe the system, and when the Hamiltonian is time independent we use TISE to describe the system. However in the latter the wavefunctions are not the solution of the TISE. How can we use TDSE in a system where the Hamiltonian is time independent?
 
  • #13
Physicslad00 said:
When the Hamiltonian is time dependent, we use TDSE to describe the system, and when the Hamiltonian is time independent we use TISE to describe the system.
Not true. We use the TDSE in both cases. When the Hamiltonian is time-independent, we may additionally use the TISE as a convenient tool for intermediate calculations.
 
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  • #14
Physicslad00 said:
What I can't understand is the significance of Hamiltonian being time independent.
If you can't understand it, then you should not make definitive statements like this...

Physicslad00 said:
When the Hamiltonian is time dependent, we use TDSE to describe the system, and when the Hamiltonian is time independent we use TISE to describe the system.
...particularly when they are wrong. And even more particularly when you have already been told they are wrong earlier in the thread.

The significance of the TISE, as has already been explained, is that it picks out a particular set of useful functions, the "stationary state" functions (more precisely, as I explained in my previous post, they are functions describing the "stationary states" at time ##t = 0##, when the phase factor ##e^{i E t}## is ##1##). That's all.
 
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  • #15
Don't cling to the terminology and try to understand the concepts (I'm mostly reiterating what has been already written above):

We have an equation which gives the time evolution of the state in all cases. This equation is what corresponds to Newton's second law in classical mechanics and it reads \partial_t |\psi \rangle = \hat H |\psi \rangle.

We also have an equation which gives the possible energies for an energy measurement and the states associated with these energies. According to the postulates of QM this is an eigenvalue equation and it reads \hat H|E_n\rangle = E_n|E_n\rangle.

A straightforward thing is to call the first equation "Schrödinger equation" (without qualifier) and the second equation "eigenvalue equation for the Hamiltonian". Since both equations involve the Hamiltonian, people sometimes use a different terminology with similar names for these very different equations (TDSE for the first and TISE for the second). If this terminology confuses you, I suggest to always think in a more straightforward terminology.

Now rephrasing your question using such a terminology: do you expect linear combinations of energy eigenvectors to be solutions of the eigenvalue equation of the Hamiltonian?
 
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  • #16
PeterDonis said:
If you can't understand it, then you should not make definitive statements like this......particularly when they are wrong. And even more particularly when you have already been told they are wrong earlier in the thread.

The significance of the TISE, as has already been explained, is that it picks out a particular set of useful functions, the "stationary state" functions (more precisely, as I explained in my previous post, they are functions describing the "stationary states" at time ##t = 0##, when the phase factor ##e^{i E t}## is ##1##). That's all.
I have read more about this topic and have come to a conclusion please tell if I am correct or not.
The state of a system is described by the wavefunction which is a solution to the TDSE. These wavefunctions are linear combination of the eigenfunctions. When the Hamiltonian is independent of time, the eigenfunctions which are the basis functions don't change with time so it becomes easy to find a general solution to the TDSE which tells us how the system evolves with time. However when the Hamiltonian is time-dependent the eigenfunctions would also be time dependent and hence finding the general solution to the TDSE would be quite difficult. However the linear combination of these time dependent eigenfunctions would still give the solution to the TDSE.
 
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  • #17
That's about right, except that if the Hamiltonian is time-dependent, then the time-dependent eigenfunctions have no relevance at all (except maybe in some approximation schemes). The time-dependent eigenfunctions don't solve the TDSE.
 
  • #18
Nullstein said:
That's about right, except that if the Hamiltonian is time-dependent, then the time-dependent eigenfunctions have no relevance at all (except maybe in some approximation schemes). The time-dependent eigenfunctions don't solve the TDSE.
so there exists no concept of stationary states in time dependent hamiltonian system?
 
  • #19
You can still possibly have stationary states, but they aren't so easy to get. You want to solve the equation ##U(t)\psi = e^{i\phi(t)}\psi##, where ##U(t)## is the time-ordered exponential of ##H(t)##. I don't think the time-dependent eigenfunctions will help you here.
 
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  • #20
In the case of time-periodic Hamiltonians there is Floquet theory which talks about certain time-periodic states, as opposed to stationary states. This comes up a lot in periodically-driven quantum systems. Section 5.3 of this write-up talks about the mathematics of these time-periodic systems.
 
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  • #21
Physicslad00 said:
The state of a system is described by the wavefunction which is a solution to the TDSE.
Yes.

Physicslad00 said:
These wavefunctions are linear combination of the eigenfunctions.
They are linear combinations of solutions of the TISE with phase factors. These are eigenfunctions of the Hamiltonian, yes. But this is only true if the Hamiltonian is time-independent; if it is not, you can't use the TISE to begin with, so you can't find any solutions of it to use as a basis to express other wave functions.

Physicslad00 said:
When the Hamiltonian is independent of time, the eigenfunctions which are the basis functions don't change with time
Not quite; they do have phase factors ##e^{i E t}##, which are functions of time. What doesn't change with time in this case is the values of observables for the eigenfunctions.

Physicslad00 said:
when the Hamiltonian is time-dependent the eigenfunctions would also be time dependent
No. As above, when the Hamiltonian is time-dependent, there is no eigenvalue equation to solve to begin with, since you can't use the TISE.
 
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  • #22
Nullstein said:
the time-dependent eigenfunctions
What time-dependent eigenfunctions? If the Hamiltonian is time-dependent, the TISE is not valid to begin with.
 
  • #23
PeterDonis said:
What time-dependent eigenfunctions? If the Hamiltonian is time-dependent, the TISE is not valid to begin with.
Why shouldn't the eigenvalue equation ##\hat{H} |\psi \rangle =E |\psi \rangle## not be valid, only because ##\hat{H}## is (explicitly) time-dependent? Of course in this case the eigenvectors are time-dependent.
 
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  • #24
PeterDonis said:
What time-dependent eigenfunctions? If the Hamiltonian is time-dependent, the TISE is not valid to begin with.
If ##H(t+\Delta t)## is a sufficiently mild perturbation of ##H(t)##, then the eigenvalues and eigenfunctions are analytic functions of ##\Delta t##, so you get time-dependent eigenfunctions. They are just not very useful, as I said.
 
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  • #25
From memory there is the wavefunction and what it interacts with - the Hamiltonian- like the infinite well problem. The wells structure doesn't change in time but it does with change in x- so the H is time independent. Not sure about relativity here.
 
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