common proposal to address the possibility of leptogenesis in A$_{4}$ models is adding A$_{4}$ soft breaking terms into Lagrangian such that the deviation of TBM as well as CP-asymmetries responsible for leptogenesis can be generated [14], while in Ref.[15–17] the authors consid- ered higher dimensional operators based on an effective theory. Instead of that, we add one 5-dimensional effective operator with respect to Λ under SU (2) × U (1) × A$_{4}$ × Z$_{2}$ × Z$_{4}$ , and A$_{4}$ × Z$_{4}$ symmetries are broken after the assuming scalars develop VEVs with ad hoc constraints in the potential $^{1}$, which opens the possibility to study an attractive mechanism of leptogenesis and to connect this with low-energy observables without contradicting 1 σ results [1]. 1 see, more details in Appendix 3 Besides the mystery of the mixing pattern, tiny neutrino mass is one of the most chal- lenging problem beyond Standard Model. Recently, E.Ma introduced the so-called radiative seesaw mechanism [18] where the neutrino masses are generated through one-loop mediated by a new Higgs doublet and right-handed neutrinos obeying an additional Z$_{2}$ symmetry. In this paper, we address the possibility of an linking between TeV-leptogenesis and non-zero θ$_{13}$ through symmetry breaking of A$_{4}$ in a radiative seesaw mechanism. Our starting point is an effective Lagrangian with an A$_{4}$ × Z$_{2}$ × Z$_{4}$ symmetry which is broken by the VEV of SU (2)$_{L}$ × U (1)$_{Y}$ singlet scalar fields at a scale higher than the electroweak scale. In addition to this, we assign a Z$_{2}$ -odd quantum number to a leptonic Higgs doublet η = ( η $^{+}$, η$^{0}$) and three right-handed singlet fermions N$_{i}$ while all the standard model particles are Z$_{2}$ -even. After electroweak symmetry breaking, the Z$_{2}$ symmetry is exactly conserved and η will not develop a VEV, that is 〈 η $^{0}$〉 = 0, while the standard Higgs boson get a VEV, which means the Yukawa coupling corresponding to Z$_{2}$ -odd Higgs doublet will not generate the Dirac mass terms in neutrino sector. Thus, the usual seesaw mechanism does not work any more and we naturally have a good candidate of dark matter (DM) corresponding to the lightest Z$_{2}$ -odd particle or Large Hadron Collider (LHC) signals through the standard gauge inter- actions in our model. The assigned leptonic flavor symmetry will lead us to the TBM, and for both its deviation and leptogenesis to be explained one A$_{4}$ triplet scalar field with cutoff scale Λ is introduced in leptonic sector. We analyze possible spectrums of light neutrinos and their flavor mixing angles. And we show that non-resonance leptogenesis at TeV-scale constrained by low energy data is achievable.