The quark–lepton complementarity (QLC) is a possible fundamental symmetry between quarks and leptons. First proposed in 1990 by Foot and Lew, it assumes that leptons as well as quarks come in three "colors". Such theory may reproduce the Standard Model at low energies, and hence quark–lepton symmetry may be realized in nature.
Possible evidence for QLC Recent neutrino experiments confirm that the Pontecorvo–Maki–Nakagawa–Sakata matrix UPMNS contains large mixing angles. For example, atmospheric measurements of particle decay yield θPMNS23 ≈ 45°, while solar experiments yield θPMNS12 ≈ 34°. Compare these results with θPMNS13 ≈ 9° which is clearly smaller, at about 1/4~1/3× the size, and with the quark mixing angles in the Cabibbo–Kobayashi–Maskawa matrix UCKM . The disparity that nature indicates between quark and lepton mixing angles has been viewed in terms of a "quark–lepton complementarity" which can be expressed in the relations
θ 12 PMNS + θ 12 CKM ≈ 45 ∘ , {\displaystyle \theta _{12}^{\text{PMNS}}+\theta _{12}^{\text{CKM}}\approx 45^{\circ }\,,}
θ 23 PMNS + θ 23 CKM ≈ 45 ∘ . {\displaystyle \theta _{23}^{\text{PMNS}}+\theta _{23}^{\text{CKM}}\approx 45^{\circ }\,.}
Possible consequences of QLC have been investigated in the literature and in particular a simple correspondence between the PMNS and CKM matrices have been proposed and analyzed in terms of a correlation matrix. The correlation matrix VM is roughly defined as the product of the CKM and PMNS matrices:
V M = U CKM ⋅ U PMNS , {\displaystyle V_{\text{M}}=U_{\text{CKM}}\cdot U_{\text{PMNS}}\,,}
Unitarity implies:
U PMNS = U CKM † V M . {\displaystyle U_{\text{PMNS}}=U_{\text{CKM}}^{\dagger }V_{\text{M}}\,.}
Open questions One may ask where the large lepton mixings come from, and whether this information is implicit in the form of the VM matrix. This question has been widely investigated in the literature, but its answer is still open. Furthermore, in some Grand Unification Theories (GUTs) the direct QLC correlation between the CKM and the PMNS mixing matrix can be obtained. In this class of models, the VM matrix is determined by the heavy Majorana neutrino mass matrix. Despite the naïve relations between the PMNS and CKM angles, a detailed analysis shows that the correlation matrix is phenomenologically compatible with a tribimaximal pattern, and only marginally with a bimaximal pattern. It is possible to include bimaximal forms of the correlation matrix VM in models with renormalization effects that are relevant, however, only in particular cases with tan β > 40 {\displaystyle \ \tan \beta >40\ } and with quasi-degenerate neutrino masses.
See also Leptoquark
Footnotes
References
Chauhan, B.C.; Picariello, M.; Pulido, J.; Torrente-Lujan, E. (2007). "Quark–lepton complementarity, neutrino and standard model data predict θPMNS13 = (9+1−2)°". European Physical Journal C. 50 (3): 573–578. arXiv:hep-ph/0605032. Bibcode:2007EPJC...50..573C. doi:10.1140/epjc/s10052-007-0212-z. S2CID 118107624. Patel, K.M. (2011). "An SO(10) × S4 Model of Quark–Lepton Complementarity". Physics Letters B. 695 (1–4): 225–230. arXiv:1008.5061. Bibcode:2011PhLB..695..225P. doi:10.1016/j.physletb.2010.11.024. S2CID 118623115.
