Positive Definite Cartan Matrices in Quantum Physics

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Discussion Overview

The discussion revolves around the properties of positive definite Cartan matrices in the context of quantum physics, particularly exploring their implications for symmetry breaking and the role of Lie groups in quantum mechanics. Participants are examining both theoretical aspects and potential physical consequences.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that the Cartan matrix they are considering is positive definite but not symmetric, questioning whether this asymmetry relates to symmetry breaks in quantum physics.
  • Another participant seeks clarification on what is meant by "symmetry breaks," suggesting various interpretations such as spontaneous symmetry breaking or phase transitions.
  • A different participant expresses curiosity about the physical consequences of the asymmetry in the Cartan matrix and its connection to the prominence of simple Lie groups in quantum mechanics, while requesting to avoid distractions related to specific groups.
  • One participant asks for clarification on what Cartan matrices are, indicating a potential gap in understanding among participants.
  • Several participants engage in a light exchange regarding the use of TeX for mathematical representation, with one providing a link to a resource on Lie algebras.

Areas of Agreement / Disagreement

The discussion contains multiple competing views and interpretations regarding the implications of Cartan matrices and symmetry breaking, with no consensus reached among participants.

Contextual Notes

Participants have not fully defined their terms or assumptions, particularly regarding the nature of symmetry breaking and the specific properties of Cartan matrices. There are also unresolved questions about the physical implications of the discussed concepts.

fresh_42
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TL;DR
Cartan Matrices are not symmetric.
As I was looking for an example for a metric tensor that isn't among the usual suspects, I observed that the Cartan matrix I wanted to use is positive definite (I assume all are), but not symmetric. Are the symmetry breaks in quantum physics related to this fact?
 
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fresh_42 said:
I observed that the Cartan matrix I wanted to use is positive definite (I assume all are), but not symmetric. Are the symmetry breaks in quantum physics related to this fact?
We'll need a bit more info on what you (think you) mean by "symmetry breaks in quantum physics". Spontaneous symmetry breaking? Pathologies at boundaries between different phases of matter? Something else?
 
I just wondered whether this asymmetry in the matrix that in the end defines a metric for mathematicians, and which I have been told years ago on PF is therefore essentially responsible that especially simple Lie groups play such a prominent role in QM, has any physical consequences and if, what they are. And please, don't open a distraction with ##U(1)## or the ##A_l## series.
 
Last edited:
What precisely are you talking about? What are "Cartan matrices"?
 
\begin{align*} A_l &: &\begin{pmatrix}2&-1&0&&& \cdots &&0 \\ -1&2&-1&0&&\cdots &&0\\ 0&-1&2&-1&0&\cdots&&0\\ \cdot&\cdot&\cdot&\cdot&\cdot&\cdots &\cdot&\cdot\\ 0&0&0&0&0&\cdots&-1&2 \end{pmatrix}\\ \\ \hline &&\\ B_l &: &\begin{pmatrix}2&-1&0&&\cdots&&&0\\ -1&2&-1&0&\cdots&&&0\\ \cdot&\cdot&\cdot&\cdot&\cdots&\cdot&\cdot&\cdot\\ 0&0&0&0&\cdots&-1&2&-2\\ 0&0&0&0&\cdots&0&-1&2 \end{pmatrix}\\ \\ \hline &&\\ C_l &: &\begin{pmatrix}2&-1&0&&\cdots&&&0\\ -1&2&-1&&\cdots&&&0\\ 0&-1&2&-1&\cdots&&&0\\ \cdot&\cdot&\cdot&\cdot&\cdots&\cdot&\cdot&\cdot\\ 0&0&0&0&\cdots&-1&2&-1\\ 0&0&0&0&\cdots&0&-2&2 \end{pmatrix}\\ \\ \hline &&\\ D_l &: &\begin{pmatrix}2&-1&0&\cdot&\cdot&\cdot&\cdot&\cdot&\cdot&0\\ -1&2&-1&\cdot&\cdot&\cdot&\cdot&\cdot&\cdot&0\\ \cdot&\cdot&\cdot&\cdot&\cdot&\cdot&\cdot&\cdot&\cdot&\cdot\\ 0&0&\cdot&\cdot&\cdot&-1&2&-1&0&0\\ 0&0&\cdot&\cdot&\cdot&\cdot&-1&2&-1&-1\\ 0&0&\cdot&\cdot&\cdot&\cdot&0&-1&2&0\\ 0&0&\cdot&\cdot&\cdot&\cdot&0&-1&0&2 \end{pmatrix}\\ \\ \hline && \end{align*}
\begin{align*} E_6 &: &\begin{pmatrix}2&0&-1&0&0&0\\ 0&2&0&-1&0&0\\ -1&0&2&-1&0&0\\ 0&-1&-1&2&-1&0\\ 0&0&0&-1&2&-1\\ 0&0&0&0&-1&2 \end{pmatrix}\\ \\ \hline &&\\ E_7 &: &\begin{pmatrix}2&0&-1&0&0&0&0\\ 0&2&0&-1&0&0&0\\ -1&0&2&-1&0&0&0\\ 0&-1&-1&2&-1&0&0\\ 0&0&0&-1&2&-1&0\\ 0&0&0&0&-1&2&-1\\ 0&0&0&0&0&-1&2 \end{pmatrix}\\ \\ \hline &&\\ E_8 &: &\begin{pmatrix}2&0&-1&0&0&0&0&0\\ 0&2&0&-1&0&0&0&0\\ -1&0&2&-1&0&0&0&0\\ 0&-1&-1&2&-1&0&0&0\\ 0&0&0&-1&2&-1&0&0\\ 0&0&0&0&-1&2&-1&0\\ 0&0&0&0&0&-1&2&-1\\ 0&0&0&0&0&0&-1&2 \end{pmatrix}\\ \\ \hline\\ F_4 &: &\begin{pmatrix}2&-1&0&0\\ -1&2&-2&0\\ 0&-1&2&-1\\ 0&0&-1&2 \end{pmatrix}\\ \\ \hline &&\\ G_2 &: &\begin{pmatrix}2&-1\\ -3&2 \end{pmatrix}\\ \\ \hline && \end{align*}
 
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