How fundamental are complex numbers in quantum theory?

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Discussion Overview

The discussion revolves around the role of complex numbers in quantum mechanics (QM), exploring whether QM could have been formulated using real-valued quantities instead. Participants examine the historical context of complex numbers in QM, the implications of alternative mathematical frameworks like Hartley analysis, and the necessity of complex numbers for representing quantum phenomena, particularly in terms of amplitude and phase.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that the use of complex numbers in QM is inherited from Fourier analysis, questioning if real-valued formulations could suffice instead.
  • Others argue that the Hartley transform lacks the ability to convey phase information, which is crucial for quantum interference, thus limiting its applicability in QM.
  • A few participants propose that QM could potentially be expressed using real numbers or through alternative mathematical constructs like Clifford algebra.
  • One participant mentions that certain solutions in quantum theory can be represented using real functions, indicating that real numbers may have more utility in QM than commonly perceived.
  • Concerns are raised about the interpretation of measurement outcomes in QM, specifically regarding how they can be mathematically represented by real numbers.
  • There is a contention about whether the Hartley transform can be adapted to replace complex numbers, with some asserting that no straightforward method exists for this substitution.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the necessity and fundamental nature of complex numbers in quantum mechanics. The discussion remains unresolved, with no consensus on whether QM could be effectively formulated without them.

Contextual Notes

Some arguments depend on specific interpretations of mathematical constructs and their implications for quantum theory, which may not be universally accepted. The discussion also highlights the limitations of the Hartley transform in conveying phase information compared to Fourier analysis.

Guillemet
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The initial development of QM inherited the use of complex numbers from Fourier analysis. Had Hartley analysis been invented first, is it possible that QM might have been formulated in terms of real-valued quantities instead, or are complex numbers in some sense natural or necessary when describing quantum phenomena?
 
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Guillemet said:
The initial development of QM inherited the use of complex numbers from Fourier analysis. Had Hartley analysis been invented first, is it possible that QM might have been formulated in terms of real-valued quantities instead, or are complex numbers in some sense natural or necessary when describing quantum phenomena?

Try this:

http://arxiv.org/abs/0907.0909
 
Interesting, but it seems to assume a priori the use of 2-dimensional quantities of some sort, though not complex numbers specifically. Has anyone devised a similar argument that rules out the reals?
 
Guillemet said:
Had Hartley analysis been invented first

Can you provide a reference about this? A Google search for "Hartley analysis" yields only pages about the British writer L. P. Hartley, as far as I can tell (clicking through five pages of search results). Nothing to do with mathematics.
 
jtbell said:
Can you provide a reference about this?
Wikipedia: Hartley transform
jtbell said:
A Google search for "Hartley analysis" yields only pages about the British writer L. P. Hartley, as far as I can tell (clicking through five pages of search results). Nothing to do with mathematics.
Weird, I get three math-related matches on the first page: http://ieeexplore.ieee.org/xpls/abs_all.jsp?arnumber=272142 http://dx.doi.org/10.1109/CIC.1989.130514 http://www-hsc.usc.edu/~jadvar/CinC-Cepstrum.pdf
 
Last edited by a moderator:
See this thread about writing the Schrödinger equation as two real differential equations.
 
I see nothing fundamental about complex numbers; quantum mechanics can be expressed just as well in the language of 2-d vectors (where vector addition corresponds to complex addition, and complex multiplication corresponds to adding up angles and multiplying lengths).

Bottom line is, you need a system of encoding 'amplitude' and 'phase'. Both are important. Phase is important because it enables interference to take place.

The Hartley transform does not give you the phase information, so no, I don't see any (obvious) way that quantum mechanics could be adapted to use Hartley analysis instead, though it might be possible through some non-obvious method.
 
Guillemet said:
The initial development of QM inherited the use of complex numbers from Fourier analysis. Had Hartley analysis been invented first, is it possible that QM might have been formulated in terms of real-valued quantities instead, or are complex numbers in some sense natural or necessary when describing quantum phenomena?

As I wrote several times in this forum, a lot more can be done in quantum theory using just real numbers (not pairs of real numbers) than people tend to think. For example, for each solution of the Klein-Gordon equation there is a physically equivalent solution (coinciding with the original solution up to a gauge transform) with a real matter field (E. Schroedinger, Nature (London) 169, 538 (1952) ). Furthermore, in a general case, the Dirac equation can be rewritten as an equation for just one real function (http://akhmeteli.org/wp-content/uploads/2011/08/JMAPAQ528082303_1.pdf , published in Journ. Math. Phys.).
 
  • #10
I found very interesting and illuminating the paper posted by "Friend". I have one doubt. What are your interpretations of the following, and perhaps more important, statement of that paper:

"each sequence of measurement outcomes obtained in a given experiment is represented
by a pair of real numbers"

I have an obvious intuition but I am searching for a precise (mathematical) definition of what the word "represented" means. Something like "a sequence of measurement outcomes is said to be represented by a mathematical object when ..."

Any thoughts would be very welcome.
 
  • #11
IttyBittyBit said:
Bottom line is, you need a system of encoding 'amplitude' and 'phase'. Both are important. Phase is important because it enables interference to take place.

The Hartley transform does not give you the phase information, so no, I don't see any (obvious) way that quantum mechanics could be adapted to use Hartley analysis instead, though it might be possible through some non-obvious method.

Hartley and Fourier both give phase spectra.
 
  • #12
Guillemet said:
Hartley and Fourier both give phase spectra.

Nope, Hartley doesn't. Each Fourier coefficient encodes the amplitude and phase of the specified frequency, whereas to determine phases in the Hartley transform you need to look at all the coefficients together (using cepstral methods for example). In other words, the transform does not directly give you the phase information.

As an example, you can consider a gabor function (sinusoid multiplied by gaussian). The Fourier transform would be a peak at the frequency of the sinusoid which falls off as a gaussian curve. The phase of the peak in the frequency domain tells you the offset of the function in the time domain. The magnitude of the peak tells you the amplitude of the signal. The Hartley transform of this function has a similar structure to the real part of the Fourier transform, BUT the height of the peak is no longer independent of phase.

As I said, there might be some convoluted method to get Hartley analysis to work as a substitute for complex numbers. There is no obvious or straightforward way, though.
 

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