same time, one may argue that the dimensionless coefficients (that are present in the kinetic-like terms of (\[theory\_L\_even\_lepton\])–(\[theory\_L\_odd\_photon\])) do not actually play a dominant role when considering any high-energy processes unless going into the Planck-scale physics (this differs significantly from the viewpoint accepted in [@Altschul]). In fact, it is believed that the scale that governs the values of the SME-specific parameters is the Planck scale, namely, the Planck mass $ M_{P} \simeq 1.22 \cdot 10^{28} \, \text{eV} $. This implies that coefficients with higher mass dimensions have to possess additional factors of $ M_{P} $ with respect to the others [@sme_theory]. It is obvious then that the Lagrangian terms containing the coefficients with the highest possible mass dimensions (i.e., $ mass^{1} $) are of primary importance for a particle with a given energy $ E \ll M_{P} $ since they do not involve any derivatives. In particular, if one has the relation $ | b_{\mu} | \sim M_{P} \, | c_{\mu \nu} | $ for the characteristic scales of the parameters $ b_{\mu} $ and $ c_{\mu \nu} $ then the average values of the corresponding Lagrangian terms are related as follows: $ | {\langle}i \gamma^{\mu} c_{\mu \nu} D^{\nu} {\rangle}| 