Is Non-Commutative Geometry the Key to a Discrete Model of Spacetime?

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    Discrete Physics Theory
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Discussion Overview

The discussion centers around the concept of whether physics could fundamentally be discrete, exploring theories that incorporate discrete mathematics as foundational elements, with quantum mechanics (QM), general relativity (GR), and differential equations emerging from this framework. The conversation touches on various theoretical approaches, including non-commutative geometry and lattice gauge theory.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that physics could be fundamentally discrete and are seeking notable theories that support this idea.
  • One participant mentions lattice gauge theory and finite difference methods as discrete approaches but questions their relevance to the idea of discreteness as a fundamental feature.
  • Another participant shares a perspective from a professor suggesting that differentiability may be an approximation of underlying discrete phenomena, although this view is noted as philosophical and not the focus of the discussion.
  • A participant argues that if spacetime is discrete, it cannot simply be pixelized, as this would violate Lorentz invariance and be observer dependent. They suggest non-commutative geometry as a potential framework for a discrete model of spacetime.
  • The concept of a "fuzzy sphere" is introduced as an example of how area can be discretized in a way that remains observer independent, with the continuous surface emerging as a limit.

Areas of Agreement / Disagreement

Participants express varying viewpoints on the nature of discreteness in physics, with some supporting the idea of discrete models while others challenge the applicability of certain existing theories. The discussion remains unresolved, with multiple competing views presented.

Contextual Notes

There are limitations regarding the assumptions made about the nature of spacetime and the definitions of discreteness versus continuity. The discussion also reflects a range of interpretations of mathematical methods and their implications for physical theories.

waves and change
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Physics could be fundamentally discrete. Are their any notable theories that have discrete mathematics at its core and have QM, GR and differential equations in general as emergent features?
 
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Thank you !
 
waves and change said:
Thank you !

Finite difference method is just a discrete method to approximate a diff. Equation. That doesn’t really give any insight into my question as posing discreteness as the underlying fundamental feature. Same can be said for Lattice gauge theory which just serves as a tool to approximation continuity
 
waves and change said:
Finite difference method is just a discrete method to approximate a diff. Equation.
I knew a professor who saw it the other way around: "Since there is nothing really continuous in the world out there, differentiabilty is an approximation of the discrete things which happen!" O.k. he mainly meant it to motivate the drawings of vector fields, but anyhow, there is some truth in it.

P.s.: I mentioned this as a contradictory possible statement, not to start a discussion upon. This belongs into philosophy and will not be dealt with on PF. However, I couldn't let stand this extreme claim as only possible truth. It is not.
 
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waves and change said:
Physics could be fundamentally discrete. Are their any notable theories that have discrete mathematics at its core and have QM, GR and differential equations in general as emergent features?

Many people are working along these lines, but it is not simple. If spacetime is discrete, for example, it cannot simply be pixelized like the pixels on your display screen, because this would not be Lorentz invariant and would be observer dependent. An attempt to formulate a discrete model of spacetime, which I personally believe is in the right direction, is to use non-commutative geometry. This draws on the idea of quantum phase space, where the coordinates (x and px, ...) do not commute and the volume of quantum phase space is basically discrete in units of (2 π ħ)^3. An example that helped me to understand these ideas is that of the "fuzzy sphere", where the area of the sphere is discretized into N units (where N can be any integer from 2 on up) in a way that is observer independent. As N goes to infinity, one recovers the usual continuous spherical surface.
 
phyzguy said:
Many people are working along these lines, but it is not simple. If spacetime is discrete, for example, it cannot simply be pixelized like the pixels on your display screen, because this would not be Lorentz invariant and would be observer dependent. An attempt to formulate a discrete model of spacetime, which I personally believe is in the right direction, is to use non-commutative geometry. This draws on the idea of quantum phase space, where the coordinates (x and px, ...) do not commute and the volume of quantum phase space is basically discrete in units of (2 π ħ)^3. An example that helped me to understand these ideas is that of the "fuzzy sphere", where the area of the sphere is discretized into N units (where N can be any integer from 2 on up) in a way that is observer independent. As N goes to infinity, one recovers the usual continuous spherical surface.

Thank you. I will look into this!
 

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