Beyond one-loop calculation: Higher-order effects on Gross-Neveu-Yukawa tensorial criticality

We study the Gross-Neveu-Yukawa field theory for the SO($N$) symmetric traceless rank-two tensor order parameter coupled to Majorana fermions using the $\epsilon$-expansion around upper critical dimensions of $3+1$ to two loops. Previously we established in the one-loop calculation that the theory does not exhibit a critical fixed point for $N \geq 4$, but that nevertheless the stable fixed point inevitably emerges at a large number of fermion flavors $N_f$. For $N_f < N_{f,c1} \approx N/2$, no critical fixed point exists; for $N_{f,c1} < N_f < N_{f,c2}$, a real critical fixed point emerges from the complex plane but fails to satisfy the additional stability conditions necessary for a continuous phase transition; and finally only for $N_f > N_{f,c2} \approx N$, the fixed point satisfies the stability conditions as well. In the present work we compute the $O(\epsilon)$ (two-loop) corrections to the critical flavour numbers $N_{f,c1}$ and $N_{f,c2}$. Most importantly, we observe a sharp decrease in $N_{f,c2}$ from its one-loop value, which brings it closer to the point $N_f =1$ relevant to the standard Gross-Neveu model. Some three-loop results are also presented and discussed.