Magnetic properties of a metal-organic antiferromagnet on a distorted honeycomb lattice
Ivan Spremo, Florian Schuetz, Peter Kopietz, Volodymyr Pashchenko,, Bernd Wolf, Michael Lang, Jan W. Bats, Chunhua Hu, Martin U. Schmidt

TL;DR
This study investigates the magnetic behavior of a metal-organic antiferromagnet on a distorted honeycomb lattice at high temperatures, revealing how its properties can be modeled by a modified spin-wave theory.
Contribution
It provides the first detailed analysis of the magnetic properties of Mn-based metal-organic antiferromagnets on a distorted honeycomb lattice using a modified spin-wave approach.
Findings
Magnetic susceptibility and magnetization data are well explained by the model.
The exchange couplings are approximately J2 ≈ 2J1 ≈ 1.8K.
The model accounts for the absence of spontaneous staggered magnetization at finite temperatures.
Abstract
For temperatures T well above the ordering temperature T*=3.0+-0.2K the magnetic properties of the metal-organic material Mn[C10H6(OH)(COO)]2x2H20 built from Mn^2+ ions and 3-hydroxy-2-naphthoic anions can be described by a S=5/2 quantum antiferromagnet on a distorted honeycomb lattice with two different nearest neighbor exchange couplings J2 \approx 2J1 \approx 1.8K. Measurements of the magnetization M(H,T) as a function of a uniform external field H and of the uniform zero field susceptibility \chi(T) are explained within the framework of a modified spin-wave approach which takes into account the absence of a spontaneous staggered magnetization at finite temperatures.
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