{"title":"Exploring the substitution effect on the magnetic coupling of tetrazinyl-bridged Ln2 single-molecule magnets","authors":"Niki Mavragani, Alexandros Kitos, Gayfullina Rezeda, Akseli Mansikkamäki, Jani Moilanen, Muralee Murugesu","doi":"10.1039/d4qi02796e","DOIUrl":null,"url":null,"abstract":"The design of new radical bridging ligands that can effectively promote strong magnetic coupling with Ln(III) ions needs to focus on radicals that are susceptible to synthetic modifications and bear diffuse spin density on their donor atoms. To probe this, we introduced various substituents possessing different electron-withdrawing/donating capabilities into the redox active s-tetrazinyl centre. This allowed for the systematic tuning of the redox and optoelectronic properties of the tetrazinyl ring. The effect of the substitution on the strength of the Ln-rad magnetic coupling was investigated on a series of radical-bridged Ln metallocene complexes featuring the 3,6-dimethyl-1,2,4,5-tetrazine (dmtz) and the 3,6-dimethoxy-1,2,4,5-tetrazine (dmeotz); [(Cp*2Ln)2(dmtz•-)(THF)2][BPh4]·THF (Ln = Gd (1-Gd) or Dy (1-Dy); Cp* = pentamethylcyclopentadienyl; THF = tetrahydrofuran) and [(Cp*2Ln)2(dmeotz•-)(THF)][BPh4] (Ln = Gd (2-Gd) or Dy (2-Dy)). Cyclic voltammetry, UV-Vis absorption spectroscopy, SQUID magnetometry, as well as ab initio and density functional theory (DFT) calculations are combined to underline the trends observed in this study, while comparisons to the unsubstituted 1,2,4,5-tetrazine (tz) and the 3,6-dichloro-1,2,4,5-tetrazine (dctz) are made. Notably, an intricate interplay between orbital overlap, ligand substituent effects, and changes in the coordination environment is found to collectively dictate the magnitude of JGd-rad in the investigated systems. The strong magnetic coupling combined with the highly anisotropic DyIII ions, grant 1-Dy and 2-Dy with slow magnetic relaxation in the absence of an external applied field. For 1-Dy an opening of the hysteresis loop is observed with Hc = ~5000 Oe, one of the highest coercivities for a dinuclear organic radical-bridged single-molecule magnet.","PeriodicalId":79,"journal":{"name":"Inorganic Chemistry Frontiers","volume":"52 1","pages":""},"PeriodicalIF":6.1000,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Inorganic Chemistry Frontiers","FirstCategoryId":"92","ListUrlMain":"https://doi.org/10.1039/d4qi02796e","RegionNum":1,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
引用次数: 0
Abstract
The design of new radical bridging ligands that can effectively promote strong magnetic coupling with Ln(III) ions needs to focus on radicals that are susceptible to synthetic modifications and bear diffuse spin density on their donor atoms. To probe this, we introduced various substituents possessing different electron-withdrawing/donating capabilities into the redox active s-tetrazinyl centre. This allowed for the systematic tuning of the redox and optoelectronic properties of the tetrazinyl ring. The effect of the substitution on the strength of the Ln-rad magnetic coupling was investigated on a series of radical-bridged Ln metallocene complexes featuring the 3,6-dimethyl-1,2,4,5-tetrazine (dmtz) and the 3,6-dimethoxy-1,2,4,5-tetrazine (dmeotz); [(Cp*2Ln)2(dmtz•-)(THF)2][BPh4]·THF (Ln = Gd (1-Gd) or Dy (1-Dy); Cp* = pentamethylcyclopentadienyl; THF = tetrahydrofuran) and [(Cp*2Ln)2(dmeotz•-)(THF)][BPh4] (Ln = Gd (2-Gd) or Dy (2-Dy)). Cyclic voltammetry, UV-Vis absorption spectroscopy, SQUID magnetometry, as well as ab initio and density functional theory (DFT) calculations are combined to underline the trends observed in this study, while comparisons to the unsubstituted 1,2,4,5-tetrazine (tz) and the 3,6-dichloro-1,2,4,5-tetrazine (dctz) are made. Notably, an intricate interplay between orbital overlap, ligand substituent effects, and changes in the coordination environment is found to collectively dictate the magnitude of JGd-rad in the investigated systems. The strong magnetic coupling combined with the highly anisotropic DyIII ions, grant 1-Dy and 2-Dy with slow magnetic relaxation in the absence of an external applied field. For 1-Dy an opening of the hysteresis loop is observed with Hc = ~5000 Oe, one of the highest coercivities for a dinuclear organic radical-bridged single-molecule magnet.