Abstract
The CAM (Composition-Algebra based Methodology) (Wolk in Int J Mod Phys A 35:2050037–2050075, 2020; Pap Phys 9:090002–09007, 2017; Phys Scr 94:025301–025307, 2019; Adv Appl Clifford Algebras 27(4):3225–3234, 2017; J Appl Math Phys 6:1537–1538, 2018; Phys Scr 94:105301–105306, 2019; Adv Appl Clifford Algebras 30:4–14, 2020) [46,47,48,49,50,51,52] gauge model’s fiber bundle framework—previously shown to induce the SU(2) and U(1) Lagrangians of the Standard Model—is extended to the SU(3) Lagrangian.
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Notes
The Composition Algebra-based Methodology (CAM) as set forth in References [46,47,48,49,50,51,52] and shown to be a gauge theory [52]. Composition algebras are algebras \(\mathbb {A}\) such that for any two elements the algebraic norm of their product equals the product of their norms [12, 25, 36]: \(\left\| xy\right\| =\left\| x\right\| \left\| y\right\| \;\forall x,y\in \mathbb {A}\). These composition algebras exist in 1, 2, 4 and 8 dimensions, corresponding to \(\mathbb {K}=\left\{ \mathbb {R},\mathbb {C},\mathbb {H},\mathbb {O}\right\} \) and their split versions \(\mathbb {K}^{\prime }=\left\{ \mathbb {C}^{\prime },\mathbb {H}^{\prime },\mathbb {O}^{\prime }\right\} \) [12, 35]. The \(\mathbb {K}\) algebras are the only division algebras (composition algebras without zero divisors) [12, 36].
Excepting use of, so far, \(S^{0}=\left\{ -1,1\right\} \), which is trivially isomorphic to the unit reals [9].
Ref. [31, Preface].
Ref. [31, p. 2].
See Ref. [52, Sect. 8] for further discussion of this topic.
Where we note that \(S_{\mathbb {O}_{u}}^{7}\rightarrow {\mathscr {S}}^{7}\) signifies that the unit 7-sphere with smooth octonionic operator structure \(S_{\mathbb {O}_{u}}^{7}\) now acts as an operator fiber \({\mathscr {S}}^{7}\), as with \(S_{\mathbb {H}_{u}}^{3}\rightarrow {\mathscr {S}}^{3}\) and \(S_{\mathbb {C}_{u}}^{1}\rightarrow {\mathscr {S}}^{1}\) for the SU(2) and U(1) interactions, respectively [52].
See Ref. [52, Sect. 5.3] for further discussion of the wedge action. The algebraic-topological wedge operation \(\vee \) identifies distinct points on two or more manifolds to a single point. Thus for example \(S^{1}\vee S^{1}\) is equivalent to a figure-eight—being two circles touching at a point [21]. The \(\vee \)-operation in effect connects or couples manifolds together at a common point.
See Ref. [52, Sects. 5.4.1& 5.5] for \(B_{1}\) and \(B_{3}\).
Ref. [1, Chap. 3 & Sect. 3.3].
Ref. [52, Sect. 5].
Ref. [52, Sect. 5.6].
The requirement of complexification with \(\mathrm {i}\in \mathbb {C}\) was previously addressed [52].
Ref. [52, Sects. 5.5 and 5.6].
Ref. [50, Sect. 2.2.1, Eqs. (11)–(14)].
In analogous manner as a vector space \(\mathrm {V}\) is complexified with \(\mathbb {C}\)-unit \(\mathrm {i}\): \(\mathrm {V}\overset{\otimes \mathrm {i}}{\rightarrow }\mathcal {\mathbb {V}}\) (See Ref. [34, Sect. 8.2.2)].
See Ref. [52, Sects. 5.1 & 9.3.1].
Ref. [18, Eq. (10.84)].
Ref. [6, Eqs. (9.29)–(9.30)].
See Ref. [46, Sect. III] for producing the linear portion of \(G_{\mu \nu }\).
Ref. [46, Sect. ii, Eq. (9)].
Ref. [18, pp. 235–236].
Ref. [27, Sect. 4.5].
Ref. [50, Sects. 2.2.2 & 3].
Ref. [50, Sect. 2.2.2].
Unlike for the electric and strong interactions; e.g., the electron does not strongly interact and the neutrino does not electrically interact.
Ref. [50, Sect. 2.2.2].
Ref. [18, Eq. (10.36)].
Ref. [41, Sect. 7.8.2].
Ref. [40, Sect. 4.8.6].
See Ref. [50, Sect. 2.2.2].
See Ref. [41, p. 154].
Ref. [52, Sects. 5.5–5.6].
See Ref. [50, Sect. 2.2.2].
According to the equivalence principle [7, 8, 37, 44, 45], locally flat space-time inertial frame \(\left( \mathbb {M},\eta \right) \) is recoverable in a sufficiently small neighborhood of any space-time point \(p\in (\mathbb {B},{\mathbf {g}})\) (See Ref. [7, Sect. 5.2.2 (p. 88) & Sect. 6.1.1 (p. 102)]; Ref. [37, Sects. 16 & 51)].
See Ref. [52, Secs. 5.5–5.6] for analogous formalisms of SU(2) and U(1).
Ref. [52, Eqs. (28)–(33)].
Ref. [52, Sect. 9].
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Wolk, B.J. The Underlying Fiber Bundle Geometry of the CAM Gauge Model of the Standard Model of Particle Physics: \(\pmb {SU(3)}\). Adv. Appl. Clifford Algebras 31, 26 (2021). https://doi.org/10.1007/s00006-021-01127-6
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DOI: https://doi.org/10.1007/s00006-021-01127-6
Keywords
- Clifford algebras
- Division algebras
- Gauge theory
- Parallelizable spheres
- Standard Model
- Strong interaction
- SU(3)
- Yang–Mills theory