Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study

Based on comprehensive experimental and quantum-theoretical investigations, we identify Sn0.9Fe3.1N as a canonical spin glass and the first ternary iron nitride with a frustrated spin ground state. Sn0.9Fe3.1N is the end member of the solid solution SnxFe4−xN (0 < x ≤ 0.9) derived from ferromagne...

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Main Authors: Tanja Scholz, Richard Dronskowski
Format: Article
Language:English
Published: AIP Publishing LLC 2016-05-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4948984
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spelling doaj-7b9bda1fae4f4052a584e6a4a1451a332020-11-25T01:06:13ZengAIP Publishing LLCAIP Advances2158-32262016-05-0165055107055107-1110.1063/1.4948984026605ADVSpin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical studyTanja Scholz0Richard Dronskowski1Institute of Inorganic Chemistry, RWTH Aachen University, 52056 Aachen, GermanyInstitute of Inorganic Chemistry, RWTH Aachen University, 52056 Aachen, GermanyBased on comprehensive experimental and quantum-theoretical investigations, we identify Sn0.9Fe3.1N as a canonical spin glass and the first ternary iron nitride with a frustrated spin ground state. Sn0.9Fe3.1N is the end member of the solid solution SnxFe4−xN (0 < x ≤ 0.9) derived from ferromagnetic γ′-Fe4N. Within the solid solution, the gradual incorporation of tin is accompanied by a drastic weakening of the ferromagnetic interactions. To explore the dilution of the ferromagnetic coupling, the highly tin-substituted Sn0.9Fe3.1N has been magnetically reinvestigated. DC magnetometry reveals diverging susceptibilities for FC and ZFC measurements at low temperatures and an unsaturated hysteretic loop even at high magnetic fields. The temperature dependence of the real component of the AC susceptibility at different frequencies proves the spin-glass transition with the characteristic parameters Tg  =  12.83(6) K, τ* = 10−11.8(2) s, zv = 5.6(1) and ΔTm/(Tm ⋅ Δlgω) = 0.015. The time-dependent response of the magnetic spins to the external field has been studied by extracting the distribution function of relaxation times g(τ, T) up to Tg from the complex plane of AC susceptibilities. The weakening of the ferromagnetic coupling by substituting tin into γ′-Fe4N is explained by the Stoner criterion on the basis of electronic structure calculations and a quantum-theoretical bonding analysis.http://dx.doi.org/10.1063/1.4948984
collection DOAJ
language English
format Article
sources DOAJ
author Tanja Scholz
Richard Dronskowski
spellingShingle Tanja Scholz
Richard Dronskowski
Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study
AIP Advances
author_facet Tanja Scholz
Richard Dronskowski
author_sort Tanja Scholz
title Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study
title_short Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study
title_full Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study
title_fullStr Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study
title_full_unstemmed Spin-glass behavior of Sn0.9Fe3.1N: An experimental and quantum-theoretical study
title_sort spin-glass behavior of sn0.9fe3.1n: an experimental and quantum-theoretical study
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2016-05-01
description Based on comprehensive experimental and quantum-theoretical investigations, we identify Sn0.9Fe3.1N as a canonical spin glass and the first ternary iron nitride with a frustrated spin ground state. Sn0.9Fe3.1N is the end member of the solid solution SnxFe4−xN (0 < x ≤ 0.9) derived from ferromagnetic γ′-Fe4N. Within the solid solution, the gradual incorporation of tin is accompanied by a drastic weakening of the ferromagnetic interactions. To explore the dilution of the ferromagnetic coupling, the highly tin-substituted Sn0.9Fe3.1N has been magnetically reinvestigated. DC magnetometry reveals diverging susceptibilities for FC and ZFC measurements at low temperatures and an unsaturated hysteretic loop even at high magnetic fields. The temperature dependence of the real component of the AC susceptibility at different frequencies proves the spin-glass transition with the characteristic parameters Tg  =  12.83(6) K, τ* = 10−11.8(2) s, zv = 5.6(1) and ΔTm/(Tm ⋅ Δlgω) = 0.015. The time-dependent response of the magnetic spins to the external field has been studied by extracting the distribution function of relaxation times g(τ, T) up to Tg from the complex plane of AC susceptibilities. The weakening of the ferromagnetic coupling by substituting tin into γ′-Fe4N is explained by the Stoner criterion on the basis of electronic structure calculations and a quantum-theoretical bonding analysis.
url http://dx.doi.org/10.1063/1.4948984
work_keys_str_mv AT tanjascholz spinglassbehaviorofsn09fe31nanexperimentalandquantumtheoreticalstudy
AT richarddronskowski spinglassbehaviorofsn09fe31nanexperimentalandquantumtheoreticalstudy
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