Garett Lisi's 248-dimensional theory?

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Discussion Overview

The discussion centers around Garett Lisi's 248-dimensional theory, which attempts to reconcile quantum mechanics and general relativity using Lie groups, specifically the Largest Exceptional Lie Group E_8. Participants explore the mathematical framework of Lie groups and their applications in theoretical physics, while also questioning the validity and implications of Lisi's model.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants express interest in understanding how Lie groups function and their relevance to Lisi's theory.
  • One participant explains that Lisi uses the E_8 structure to integrate gravity and quantum mechanics, suggesting that particle interactions arise from E_8 transformations.
  • Another participant disputes the claim that Lisi's model unifies gravity and quantum mechanics, arguing it violates fundamental quantum mechanical principles.
  • There is a discussion about which specific representation of the E_8 group Lisi employs, with some suggesting it is the 248 representation, which serves both as the fundamental and adjoint representation.
  • Participants explore various ways to break the E_8 symmetry and mention several subgroups that could relate to the Standard Model and other grand unified theories.
  • Questions arise regarding the specific group and algebra types used in Lisi's model, with references to global and local properties in particle physics.
  • Some participants note that the exceptional Lie algebra is likely the one being utilized in Lisi's framework.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the validity of Lisi's theory or the specifics of the E_8 representation used. There are competing views regarding the unification of gravity and quantum mechanics, as well as the implications of the E_8 structure.

Contextual Notes

Participants express uncertainty about the definitions and properties of the E_8 group and its representations, as well as the implications of using different forms of the group in the context of particle physics.

Matthewkind
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I'm sorry to be so bothersome; however, I've recently been hearing a lot of good things about this Garett Lisi person. Apparently, he can explain the fundamental forces by using Lie Groups, which is a branch of mathematics that I am currently not familiar with. I only know that it works through some sort of crazy circle distortion thing. Can anyone explain to me how Lie groups work? Also, can you explain to me exactly what Mr. Lisi is positing when he claims to have reconciled quantum mechanics and general relativity?
 
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He essentially used the Largest Exceptional Lie Group [tex]E_8[/tex] and put gravity and quantum mechanics into the [tex]E_8[/tex] structure. The transformations of [tex]E_8[/tex] structure produce the particle interactions et cetera. Particle physics already uses Lie Groups such as the Electroweak Unification uses [tex]SU(2) \otimes U(1)[/tex] which is a sub-group in the larger [tex]E_8[/tex] group. It's more of a GUT then a full theory of everything as many other problems aren't addressed and the theory is still in its infancy.

"More specifically, Lisi combines the left-right symmetric Pati-Salam GUT with a MacDowell-Mansouri description of gravity, using the spin connection and gravitational frame combined with a Higgs boson, necessitating a cosmological constant. The model is formulated as a gauge theory, using a modified BF action, with E8 as the Lie group. Mathematically, this is an E8 principal bundle, with connection, over a four dimensional base manifold. Lisi's embedding of the Standard Model gauge group in E8 leads him to predict the existence of 22 new bosonic particles at an undetermined mass scale." - Wikipedia

An example of a Lie group is a rotation in the complex plane about a circle with radius 1. This is called the [tex]U(1)[/tex] Lie group. I believe the transformations follow the equation [tex]e^{i\theta} = cos \theta+ isin\theta[/tex]

Wiki: http://en.wikipedia.org/wiki/An_Exceptionally_Simple_Theory_of_Everything
TED Talk:
Elementary Particle Explorer: http://deferentialgeometry.org/epe/EPE3.html
 
Last edited by a moderator:
Kevin_Axion said:
He essentially used the Largest Exceptional Lie Group [tex]E_8[/tex] and put gravity and quantum mechanics into the [tex]E_8[/tex] structure.

Nope, there is nothing about a unification of gravity and quantum mechanics in this model. On the contrary, it is in violation of basic quantum mechanical principles like the spin-statistics theorem.
 
Which [tex]E_8[/tex] group does he use?
 
More properly, which E8 representation does he use?

From what I gather, it's the 248 representation, which is both the fundamental one and the adjoint one.

Fundamental -- every other irreducible representation can be derived from product representations. If Xi is the rep's vector space, the product representations are Xi*Xj*Xk...

Adjoint -- the rep's vector space is the generators of the algebra. Gauge fields must be in the adjoint rep of their gauge algebra.

So gauge fields must be in the E8 248 rep.

The next larger E8 rep has size 3875, which is even worse.

For the 3D angular-momentum algebra, a.k.a. A1, B1, SU(2), SO(3), etc.:
Fundamental: spinor (spin 1/2, dimension 2)
Adjoint: vector (spin 1, dimension 3)

-

It's rather obvious that no experimentally-accessible particles have unbroken E8 gauge symmetry, so it must be broken in some way. But there are lots of ways to break E8:

D8 = SO(16)
A7*A1 = SU(8)*SU(2)
A5*A2*A1 = SU(6)*SU(3)*SU(2)
A4*A4 = SU(5)*SU(5)
D4*A3 = SO(10)*SU(4)
E6*A2 = E6*SU(3)
E7*A1 = E7*SU(2)
A8 = SU(9)

D7*U(1) = SO(14)*U(1)
A6*A1*U(1) = SU(7)*SU(2)*U(1)
A4*A2*A1*U(1) = SU(5)*SU(3)*SU(2)*U(1)
A4*A3*U(1) = SU(5)*SU(4)*U(1)
D5*A2*U(1) = SO(10)*SU(3)*U(1)
E6*A1*U(1) = E6*SU(2)*U(1)
A7*U(1) = SU(8)*U(1)

F4*G2

Some of these subgroups contain not only the Standard-Model symmetry, SU(3)*SU(2)*U(1), but also such much-discussed supersets of it as SU(5), SO(10), and E6.

The Pati-Salam model, mentioned in the OP, has symmetry SU(4)*SU(2)*SU(2) or SO(6)*SO(4)

It's a subset of SO(10), and thus, E6 and E8.
 
lpetrich said:
More properly, which E8 representation does he use?

Well, first I want to know which group.
 
What possibilities are there?
 
lpetrich said:
What possibilities are there?

There is the complex group. There are three real forms and two non trivial double covers. I am guessing he uses a real group and it is either the compact form or the split one.
 
Such global properties usually don't matter much in particle physics. What's usually important are the local properties -- the Lie algebra. That gentleman is apparently using a 248-dimensional representation, since it's the adjoint one.
 
  • #10
lpetrich said:
Such global properties usually don't matter much in particle physics. What's usually important are the local properties -- the Lie algebra.

If it is the algebra then why call it group! Then my question is which algebra of type E8 is he using?
 
  • #11
The exceptional Lie algebra, as far as I can tell.
 
  • #12
[tex]E_{8(-24)}[/tex]
http://arxiv.org/abs/1006.4908"
 
Last edited by a moderator:
  • #13
garrett said:
[tex]E_{8(-24)}[/tex]
http://arxiv.org/abs/1006.4908"

Thanks.
 
Last edited by a moderator:

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