Abstract

By using [Ru2(O2CC3H7)4Cl]n (1) as a starting material, nBu4N[Ru2(O2CC3H7)4Cl2] (nBu4N+ = tetra(n-butyl)ammonium cation) (2) and [Ru2(O2CC3H7)4(H2O)2]BF4 (3) were prepared. The lantern-type dinuclear structures with axial chloride ions or water molecules were confirmed for 2 and 3 by X-ray crystal structure analyses. The crystal structures of 2 and 3 were compared with that of 1. In the crystal of 2, there were three crystallographically different dinuclear units; the Ru–Ru distances of each unit were 2.3094(3), 2.3046(4), and 2.3034(4) Å, respectively, which were longer than those of 1 (2.281(4) Å) and 3 (2.2584 (7) Å). Temperature dependent magnetic susceptibility measurements were performed for 1 and 2 as well as 3. The effective magnetic moments (µeff) at 300 K were 3.97 (for 1), 4.00 (for 2), and 3.97 µB (for 3), respectively. The decreases in the µeff value were confirmed for all of the complexes due to the large zero-field splitting (D): D = 68 cm−1 for 1, 78 cm−1 for 2, and 60 cm−1 for 3. Cyclic voltammograms measured in CH2Cl2 with a electrolyte of nBu4N(BF4) showed the Ru25+/Ru24+ process at −0.2–−0.4 V (vs. SCE) and the Ru26+/Ru25+ one at 1.3–1.4 V (vs. SCE), of which potentials were confirmed by the DFT calculation for nBu4N[Ru2(O2CC3H7)4Cl2].

Highlights

  • There has been much interest devoted to lantern-type dinuclear complexes with a direct metal–metal (M–M) interaction giving a wide range of remarkable physical–chemical properties based on the direct M–M interaction [1,2,3,4,5]

  • By using [Ru2(O2CC3H7)4Cl]n as a starting material, nBu4N[Ru2(O2CC3H7)4Cl2] and [Ru2(O2CC3H7)4(H2O)2]BF4 were prepared. Their lantern-type dinuclear structures with axial ligands of Cl− or H2O were confirmed by X-ray crystal structure analyses

  • No important magnetic interaction was observed between the dinuclear units for the complexes

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Summary

Introduction

There has been much interest devoted to lantern-type dinuclear complexes with a direct metal–metal (M–M) interaction giving a wide range of remarkable physical–chemical properties based on the direct M–M interaction [1,2,3,4,5]. In the case of the ruthenium dinuclear complexes, the crystal. In the case of the ruthenium dinuclear complexes, the crystal structure was fifirrsstt rreeppoorrtteeddiinn11996699bbyyCCoottotonnaannddcoco-w-woorkrkeresrsfofor r[R[Ruu2(2O(O2C2CCC33HH77)44Cl]nn ((11)),, wwhere the mixed-valentt ddiirruutthheenniiuumm((III,I,III))ddininuuccleleaarr(R(Ruu252+)5+u)nuitnsiatsrealrienkliendkebdy baxyialxciahllocrhildoeridonesiotonsgitvoegaivzeigazaigg-zcahgaicnhsatirnusctruurcetuwriethwaitRhua–RCula–x–CRlaux–bRoundboanndglaenogfle12o5f.41°2,5a.4s◦s,haoswshnoiwn nScihneSmchee1m[e6]1. TTeemmppeerraattuurree--ddeeppeennddeennttmmagagnneteitcicsussucsecpetpibtiibliitlyitwy aws alastelartreerproerpteodrtfeodr [fRoru2[(ROu22C(OC23CHC73)H4C7)l4]Cn l(]1n) (b1y) TbeylsTeerleset rale.,t sahl.o, wshinogwainlgaragelazregreo-zfeierold-fsieplldittsipnlgit(tDing= (7D6.8= c7m6.−81c)mw−i1t)hwgit=h2g.1=02w.1i0thwthitehstuhpepsourpt poof rEtPoRf (EePleRct(reolnecptaroranmpaagrnaemtiacgrneesotincarnecseo)nsapneccetr)aslpdeacttara[7l ]d. STyhnethaesdisdaitniodnChoafrancteerxizcaetsisonasmount of nBu4NCl to the dinuclear units of [Ru2(O2CC3H7)4Cl]n (1) with stirring at room temperature for 24 h in dichloromethane solution gave a wwRwddocbonyiiuiiiccmttt2heRhhhh5lp+llueTooAAlum2herr5nsggixie+eddtiBBint[oroauRFFtrodddna44iufindliiri2rit1ganiun(uto)nOit.tfToThah2O1nHleaHCey)ntnn.FsCoFieiOuft3usaahrHman.mttoenT7r(otr(o)IhhooIme4ItIeoeo,(xh,IHImmIcoIeIIReItr2))htsOtteshsceeecmpo)amrmoa2emnhpm]mcppBdaetpeeporF,nrlrarua4ltedaaehtxon(t,tuxe3ufuttrn)hr2nraBeoeweeBxfuaiuaffin4naotoNxfB4dhlorriNua[cr3a2R2l4h[N44Rsyculohhi2uC2hher(ol42Oliolwddww(rtO2eioeCoiidhttd2flChhetCih6gt3lChss9Heiaittge%nn3iid7arrH)dC.rrni4niCiTO7dnnod)uhlfO4gg2oiceC]c1flitthvelr(oo1c22laiocb]o)rcgghrruo(iiwouae2vvultmmdn)eeiiltodiwiehtbaancstbeahsiaddteolarhaiifferynaasoem[qaiqeramReuumolyusdoaaveiu2svddet(eoolOeliiadodlrfrdufu2uwbC8totbtti5ywhehCfyo%reenot3e8tnHhnh5dc(ieie%7ubuoi)gsramn4rmtCeaes(fiiaanv(eb(lrIcI]cdecaImInttt,s,iiIiI(ooeoeIvI1IddnnInae))) ((cbbbCCoayamOOnneddOlOpessl)m)e((1x1ννe44aan[2s2sRyt5ym8amucl(c2maC((mOnC−Oa−O21OCl1)yO.C)sfTo)e13hHsr41.e6437Ts)56)e4h5(icHfenmacIm2caRO−t1s−s)sais21pmn]uBeadgicFnlgtνa4drersa(sy3νmteo)sntfy(hwCem2ariOatgt(hntCyOhdOae)re31Oydg4sii)ienh2ol16uodn4wcc2lotmeeo6fad−c6tr1hmt9sfho%ko−eser.e1Cl2eTfoO;tohofνrOena1is2ryiv;(smνciνpbh(aaCrrsesyeaymOmstmieOiorc((nvCa)Csel1OOdaf4oOsO5irn5a)m) t1cs1huem44etl65a−o2a51fbwacctonmmwevdre−o−e-ν11mdcsoyaaiemsnnnntfid(dtniCirocννmOtnssiyyOeevmmdde) wtc1roem4ha22−ci81ct)aih.conmTnidnhs−d1e3tisfo.coeaT2rfthaea3ecn)ntdsisontrs3ceau.otgTocsgihrhmdeiensiinstglatatrrvhteiieatobcntnhretaihorntgfeigoytdnhvriseinebgoiuroifacontlBneitoFaontr4o−tsshatokehpfeopRlBeseuFteao24ro5n−+faia1scspoap(prνreebaesa[rsy9rome]ara.(vdsCeaObdbaOinrno)dat1hda4er6bo2aaubncnomddv−ae11r-a0omn9ue0dnndcνtmis1oy0m−n19e(0iCdncOrm3eO,a−w)c1t1hiio4nic2n3h5s, indicate no coordination of the ion to the Ru25+ core [9]

Crystal Structures
Materials and Methods
Syntheses of Complexes
Crystal Structure Determination
Computational Details
Conclusions
Full Text
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