De Broglie Waves and Complex Numbers

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Discussion Overview

The discussion revolves around the necessity and implications of using complex numbers in quantum mechanics, particularly in relation to the wave function and the Schrödinger equation. Participants explore theoretical, mathematical, and conceptual aspects of this topic.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that complex numbers are essential in quantum mechanics due to the nature of the Schrödinger equation, which they argue has intrinsic complex solutions.
  • Others propose that while complex numbers are used for convenience, there are alternative formulations of quantum mechanics that do not require them.
  • A participant explains that the wave function must be periodic to persist, which they argue necessitates the inclusion of an imaginary component.
  • Another participant challenges the assertion that wave functions must be complex, providing examples such as the particle in a box and the harmonic oscillator, which can have real solutions.
  • Some participants discuss the implications of energy conservation and invariance under time transformation, suggesting that these physical considerations may necessitate complex solutions.
  • A later reply introduces the concept of spin and orthogonality in quantum states, arguing that complex space allows for a richer structure in describing these states.

Areas of Agreement / Disagreement

Participants express differing views on whether complex numbers are fundamentally necessary in quantum mechanics. Some argue for their necessity based on mathematical and physical reasoning, while others contend that they are merely a convenient choice without intrinsic necessity. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Participants note that the discussion involves various interpretations of the Schrödinger equation and its solutions, as well as the implications of linearity and boundary conditions. There are also references to specific examples that challenge the necessity of complex wave functions.

Xeinstein
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We used complex variables to describe the wave function. People do that in acoustics and optics too, strictly for convenience, because the real and imaginary parts are rudundant.

The wave function of quantum mechanics is "necessarily" complex, it's not just for convenience that we use complex numbers in quantum theory. Is there any physical reason for the wave function to be complex?
 
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I think there is more than one way to answer this question. One way to see that complex numbers are built into the theory rather than simply for convenience like your earlier examples is that Schrödinger's equation is a heat equation with imaginary dispersion coefficient. Thus the solutions are intrinsically complex.

The real and imaginary parts of these solutions would also obey the Schrödinger equation since the equation is linear, but they do not generally also match the boundary conditions, and are therefore not generally solutions to your physical systems (UNLIKE your counterexamples of acoustics and optics).

For a concrete example: a "left-moving particle" has a wavefunction e^{ikx}, NOT cos(kx) or sin(kx).

That might not be what you call a "physical reason", but it is a mathematical one.
 
I'll attempt an explanation without using equations.

The wave function represents the state of the system. Because its time and space derivatives must be proportional to the wave function itself, it takes an exponential form. If the argument in the exponent is real, the wave function will either grow without limit or decay away. If we want the system to persist, we need to make the wave function periodic, and that requires an i in the argument.

By the way, de Broglie waves don't have to be complex, but Schroedinger waves do. The Schroedinger equation contains an explicit i.
 
country boy said:
The wave function represents the state of the system. Because its time and space derivatives must be proportional to the wave function itself, it takes an exponential form. If the argument in the exponent is real, the wave function will either grow without limit or decay away. If we want the system to persist, we need to make the wave function periodic, and that requires an i in the argument.

By the way, de Broglie waves don't have to be complex, but Schroedinger waves do. The Schroedinger equation contains an explicit i.

Could you expand on the 'must be' please? Why must they be?
 
epenguin said:
Could you expand on the 'must be' please? Why must they be?

For example, if the energy is constant, the time derivative of the wave function is proportional to the energy multiplied by the wave function (the eigenvalue equation).

If we are going to use wave functions to describe motion, then they must be complex.
 
epenguin said:
Could you expand on the 'must be' please? Why must they be?

They don't have to be. An obvious example is the particle in a box, the solutions of which are not proportional to their odd spatial derivatives. Another example is the ground state (or any state) of a simple harmonic oscillator. Another example is *any* function other than an exponential.

So, I think that he must just be saying that the Schrödinger equation is linear. But this does not mean that the solutions are always proportional to their space and time derivatives.
 
Xeinstein - there is no physical reason why complex numbers should be used in QM. If it were so, it would be equivalent to saying it only worked in German, or in base 8 arithmetic.

There are perfectly good QM's that do not use complex numbers. It is merely a (great) convenience.
 
olgranpappy said:
They don't have to be. An obvious example is the particle in a box, the solutions of which are not proportional to their odd spatial derivatives. Another example is the ground state (or any state) of a simple harmonic oscillator. Another example is *any* function other than an exponential.

So, I think that he must just be saying that the Schrödinger equation is linear. But this does not mean that the solutions are always proportional to their space and time derivatives.

You are correct, of course, wave functions do not need to be complex. I was addressing the question about why they are (when they are). But even the solutions to Schroedinger's time-independent equation that you give as examples are associated with a time-dependent factor that is complex.
 
Regarding the Schrödinger equation from a mathematical point of view it has just one derivative in time, whereas the Maxwell eqations have a second derivative in time. That's the big difference and requires the solution of Schrödingers equation to be complex.

Physically there is another reason: Energypreservation demands that the solution has to be invariant by time transformation. If the solution would be real and you replace the t by -t there is no invariancy. But by replacing the imaginary part it to -it accomplishes the requirement.

Another reason is the Spin description. The whole theory is only possible in the complex spere (For one Spin the Bloch sphere, minus the part for unity matrix). Spin eigen states have to be orthogonal and for one spin the vector has to be 2 dimensional (because there are two possibilites: Spin up and Spin down) . Further there have to be 3 eigen states and that is possible only if two are in real space and one is imaginary. So complex space enables more orthogonal eigen states.

And then and I guess what's most important: The only way to write a vector product as an integral is in complex space, namely in Quantum physics the Hilbert space. I can't remember exactely, but it has something to do with the bilinear form ...

There would be certainly more reasons ... but that's what's crossing my mind, wright now. (No guarantee that it is correct!)
 

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