2015
DOI: 10.1142/s0219498815500917
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E6, the group: The structure of SL(3, 𝕆)

Abstract: We present the subalgebra structure of sl(3, O), a particular real form of e 6 chosen for its relevance to particle physics and its close relation to generalized Lorentz groups. We use an explicit representation of the Lie group SL(3, O) to construct the multiplication table of the corresponding Lie algebra sl(3, O). Both the multiplication table and the group are then utilized to find various nested chains of subalgebras of sl(3, O), in which the corresponding Cartan subalgebras are also nested where possible… Show more

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Cited by 7 publications
(11 citation statements)
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References 12 publications
(25 reference statements)
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“…ξm, ] ⊂ ξ 2 p = (−1)p (8) then p ⊕ ξm also has real structure constants, and is therefore also a real form of the complex Lie algebra g C . Note that φ * is a vector space isomorphism, but not a Lie algebra isomorphism -as must be the case if it takes one real form to another.…”
Section: Graded Lie Algebrasmentioning
confidence: 99%
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“…ξm, ] ⊂ ξ 2 p = (−1)p (8) then p ⊕ ξm also has real structure constants, and is therefore also a real form of the complex Lie algebra g C . Note that φ * is a vector space isomorphism, but not a Lie algebra isomorphism -as must be the case if it takes one real form to another.…”
Section: Graded Lie Algebrasmentioning
confidence: 99%
“…A description of the group E 6(−26) as SL(3, O) was given in [5], generalizing the interpretation of SL(2, O) as (the double cover of) SO(9, 1) discussed in [6]. An interpretation combining spinor and vector representations of the Lorentz group in 10 spacetime dimensions was described in [7], and in [8] we obtained nested chains of subgroups of SL (3, O) that respect this Lorentzian structure.…”
Section: Introductionmentioning
confidence: 99%
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