Is there any way to get a geometrical description of QM

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The discussion centers on the challenge of obtaining a geometrical description of quantum mechanics (QM) in three-dimensional space, as opposed to Hilbert Space. Participants highlight that while classical mechanics can provide such descriptions, QM fundamentally resists this due to its reliance on wave functions and complex numbers. The closest approximation to a geometrical representation in QM is through geometric quantization and visualizations of atomic orbits, yet these are inherently incomplete. The conversation also references Bell inequalities, which suggest limitations in achieving a classical-like description of quantum phenomena.

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  • Understanding of quantum mechanics principles, particularly wave functions
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nashed
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This is maybe one of my greatest gripes with QM, I have never seen a geometrical description of it.

What I mean by geometrical, is a description of the given object in the 3D world we live in, not a description in Hilbert Space, is such a description even possible in principle? I've been studying about Bell inequalities and they seem to suggest that maybe not, but I figured I might as well ask.
 
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nashed said:
This is maybe one of my greatest gripes with QM, I have never seen a geometrical description of it.

What I mean by geometrical, is a description of the given object in the 3D world we live in, not a description in Hilbert Space, is such a description even possible in principle? I've been studying about Bell inequalities and they seem to suggest that maybe not, but I figured I might as well ask.

Can you have such a description in classical mechanics?
 
In classical mechanics in the Newtonian formulation the "real" physical space in which the motion of material objects (such as me or the OP) is "seen" is mapped onto R^n (n=1,2 or 3) as an affine space.
 
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dextercioby said:
In classical mechanics in the Newtonian formulation the "real" physical space in which the motion of material objects (sich as me or the OP) "seen" is mapped onto R^n (n=1,2 or 3) as an affine space.

But the description of the objects in the real space, say a particle, requires you to use a different space, for a particle it's ##\mathbb R^6##.
 
Yes, as you put velocities as well. I only referred to positions.
 
martinbn said:
But the description of the objects in the real space, say a particle, requires you to use a different space, for a particle it's ##\mathbb R^6##.
Thing is, velocity is closely related to position, and eve if it's not, you've got the Newtonian formulation which happens entirely in 3D space... I'm wondering if such a formulation is even theoretically possible for QM.
 
martinbn said:
Can you have such a description in classical mechanics?

Symplectic Geometry?
https://www3.nd.edu/~eburkard/Talks/GSS%20Talk%20110413.pdf

I think the problem is the OP may not quite understand the modern conception of geometry.

Thanks
Bill
 
nashed said:
This is maybe one of my greatest gripes with QM, I have never seen a geometrical description of it. What I mean by geometrical, is a description of the given object in the 3D world we live in, not a description in Hilbert Space ...

You want a way to visualize electrons, protons etc? Classically they would be little spheres moving around under the influence of forces, like billiard balls, or planets. But in QM that picture is wrong (although not totally useless). Instead there's a wave function associated with the particle which is impossible to visualize entirely. But it can be attempted. The best examples are from chemistry. You've seen pictures of the atomic orbits of hydrogen atom, for instance? They look like spheres, barbells, etc. There are animations of such things. See this other current thread, https://www.physicsforums.com/threads/gluon-field-fluctuations.898565/, for pictures of "gluon fluctuation", a similar idea. This type of graphics represents QM functions visually (3-d). It's far from complete, leaves out essential info like (for instance) the complex nature of the wave. But it's probably about the best you can do.
 
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Doesn't the position basis do what the OP wants? The position of a particle is determined by the potential well in physical space.

Not sure I get the question, the most newb problems are defined and solved in real space, the complex numbers disappear when the complex conjugate it taken to get position, expectation value...even the integrals are defined with real space limits.
 
  • #11
The uncertainty principle can be derived by using geometrical arguments, i.e. slit experiment.
 
  • #12
nashed said:
a description of the given object in the 3D world we live in, not a description in Hilbert Space, is such a description even possible in principle?

Not for QM in general. Under conditions where the physics can be approximated classically, such a description can (usually) be given. But under conditions where a classical approximation breaks down, the ability to give a description of the kind you are talking about breaks down too. That is to be expected: QM was developed in large part because this classical type of description simply didn't work for certain phenomena.
 
  • #13
nashed said:
This is maybe one of my greatest gripes with QM, I have never seen a geometrical description of it.

What I mean by geometrical, is a description of the given object in the 3D world we live in, not a description in Hilbert Space, is such a description even possible in principle? I've been studying about Bell inequalities and they seem to suggest that maybe not, but I figured I might as well ask.
I don't know if this helps (it's a bit more complicated than need be): http://www.techlib.com/science/bells_inequality.htm
 

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