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In quasi-2D quantum magnets the ratio of Neel temperature $T_text N$ to Curie-Weiss temperature $Theta_text{CW}$ 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 $J_2/J_1$ in the whole Neel 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 $f=Theta_text{CW}/T_text N$ may be used as measure of frustration strength in the quasi-2D quantum magnets.
In-field DC and AC magnetization measurements were carried out on a sigma-phase Fe55Re45 intermetallic compound aimed at determination of the magnetic phase diagram in the H-T plane. Field cooled, M_FC, and zero-field cooled, M_ZFC, DC magnetization
We report results of muon spin relaxation and rotation ($mu$SR) experiments on the spin-liquid candidate~YbMgGaO$_{4}$. No static magnetism $gtrsim 0.003mu_B$ per Yb ion, ordered or disordered, is observed down to 22~mK, a factor of two lower in temp
Comprehensive studies of magnetic properties of GdCr3(BO3)4 single crystal have been carried out. The integrals of intrachain and interchain exchange interactions in the chromium subsystem have been determined and the strength of Cr-Gd exchange inter
Comprehensive magnetic-field-temperature ($H$-$T$) phase diagram of solid oxygen including the $theta$ phase is discussed in the context of the ultrahigh-field measurement and the magnetocaloric effect (MCE) measurement. The problems originating from
The quasi-one-dimensional antiferromagnetic Ising-like compound BaCo2V2O8 has been shown to be describable by the Tomonaga-Luttinger liquid theory in its gapless phase induced by a magnetic field applied along the Ising axis. Above 3.9 T, this leads