N\'eel temperature and reentrant H-T phase diagram of quasi-2D frustrated magnets

In quasi-2D quantum magnets the ratio of N'eel temperature $T_{\text{N}}$ to Curie-Weiss temperature ${\mathrm{\Theta }}_{\text{CW}}$ is frequently used as an empirical criterion to judge the strength of frustration. In this work we investigate how these quantities are related in the canonical quasi-2D frustrated square or triangular $J_1$-$J_2$ model. Using the self-consistent Tyablikov approach for calculating $T_{\text{N}}$ we show their dependence on the frustration control parameter $J_2\mathrm{/}{J}_1$ in the whole N'eel and columnar antiferromagnetic phase region. We also discuss approximate analytical results. In addition the field dependence of $T_{\text{N}}(H)$ and the associated possible reentrance behavior of the ordered moment due to quantum fluctuations is investigated. These results are directly applicable to a class of quasi-2D oxovanadate antiferromagnets. We give clear criteria to judge under which conditions the empirical frustration ratio $f={\mathrm{\Theta }}_{\text{CW}}\mathrm{/}{T}_{\text{N}}$ may be used as measure of frustration strength in the quasi-2D quantum magnets.