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The Underlying Fiber Bundle Geometry of the CAM Gauge Model of the Standard Model of Particle Physics: \(\pmb {SU(3)}\)

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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

  1. 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].

  2. Excepting use of, so far, \(S^{0}=\left\{ -1,1\right\} \), which is trivially isomorphic to the unit reals [9].

  3. Ref. [31, Preface].

  4. Ref. [31, p. 2].

  5. See Ref. [52, Sect. 8] for further discussion of this topic.

  6. See Ref. [52, Sects. 5.1–5.3 & 9.3.1]. The sphere \(S_{\mathbb {O}_{u}}^{7}\) has no metric defined on it—it is a smooth (differentio-topological) manifold containing the smooth division-algebraic operation (See also Ref. [52, Fn. (aaa)].

  7. 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].

  8. 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.

  9. See Ref. [52, Sects. 5.4.1& 5.5] for \(B_{1}\) and \(B_{3}\).

  10. These operators are defined in Eq. (5) below and specifically addressed in Reference [52] and throughout the CAM papers (cf. Ref. [46]).

  11. See Ref. [46, Eqs. (1)–(8)] for the \(\eta \partial \) derivation. See also Ref. [50, Sect. 2] and Ref. [47, Sect. 3.ii].

  12. Ref. [1, Chap. 3 & Sect. 3.3].

  13. Ref. [52, Sect. 7.3.2] and [49, Fn. (14) & Sect. 2.2].

  14. Refs. [50, Sect. 2.2.1], [48]. U(1) lacks the commutator and therefore its Lie algebra structure constants are identically zero.

  15. Ref. [52, Sect. 5].

  16. Ref. [52, Sect. 5.6].

  17. The requirement of complexification with \(\mathrm {i}\in \mathbb {C}\) was previously addressed [52].

  18. Ref. [52, Sects. 5.5 and 5.6].

  19. Ref. [52, Eq. (32)]; Ref. [50, Sect. 2.3].

  20. Ref. [50, Sect. 2.2.1, Eqs. (11)–(14)].

  21. 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)].

  22. Since \(\mathbb {R},\mathbb {C},\mathbb {H}\subset \mathbb {C}\ell _{1,7}\), we can write all division algebras in the form \(\mathbb {K}\oplus \ell \mathbb {K}\); e.g., \(\mathbb {H}=\mathbb {C}\oplus \ell \mathbb {C}\) [12, 35].

  23. See Ref. [52, Sects. 5.1 & 9.3.1].

  24. See Ref. [50, Eq. (2)] and references therein; Ref. [49, Eq. (9)] and references therein; Ref. [46, Eq. (6)] and references therein.

  25. Since a metric g on a manifold M is the structure that smoothly assigns to each point \(p\in M\) a metric \(g_{p}\) on \(T_{p}M\) [5, 13] by which dot and cross products manifest [5, 13, 40], the form of (15) requires operation within a manifold equipped with a metric.

  26. Ref. [18, Eq. (10.84)].

  27. Ref. [6, Eqs. (9.29)–(9.30)].

  28. See Ref. [46, Sect. III] for producing the linear portion of \(G_{\mu \nu }\).

  29. Local gauge symmetry is preserved if the fields have equal mass [41, 43].

  30. Ref. [46, Sect. ii, Eq. (9)].

  31. Ref. [18, pp. 235–236].

  32. Ref. [27, Sect. 4.5].

  33. Ref. [52, Sect. ii, Eq. (9)]. See also Ref. [49], where this structure constant constraint was shown to be the essence of why there can be no gauge-mediated proton decay via SU(5) or any other purported GUT group, and thus why such decay has never been observed.

  34. Ref. [50, Sects. 2.2.2 & 3].

  35. Ref. [50, Sect. 2.2.2].

  36. Unlike for the electric and strong interactions; e.g., the electron does not strongly interact and the neutrino does not electrically interact.

  37. Ref. [50, Sect. 2.2.2].

  38. Ref. [18, Eq. (10.36)].

  39. Ref. [41, Sect. 7.8.2].

  40. Ref. [40, Sect. 4.8.6].

  41. See Ref. [50, Sect. 2.2.2].

  42. See Ref. [41, p. 154].

  43. Ref. [52, Sects. 5.5–5.6].

  44. See Ref. [50, Sect. 2.2.2].

  45. 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)].

  46. See Ref. [52, Secs. 5.5–5.6] for analogous formalisms of SU(2) and U(1).

  47. Ref. [52, Eqs. (28)–(33)].

  48. See Ref. [18, Eq. (10.88)]; Ref. [6, Eq. (9.36)].

  49. Ref. [52, Sect. 9].

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Correspondence to Brian Jonathan Wolk.

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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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