2-吡啶甲醇和1，1，1-三羥甲基乙烷混合配體七核錳配合物的合成、晶體結構與磁性

王會生　樂琳　潘敏　鐘文達　涂偉　潘志權(武漢工程大學化學與環境工程學院，綠色化工過程教育部重點實驗室，武漢430074)

2-吡啶甲醇和1，1，1-三羥甲基乙烷混合配體七核錳配合物的合成、晶體結構與磁性

王會生＊樂琳潘敏鐘文達涂偉潘志權＊
(武漢工程大學化學與環境工程學院，綠色化工過程教育部重點實驗室，武漢430074)

四水合氯化錳、2-吡啶甲醇和1，1，1-三羥甲基乙烷在乙腈里反應合成出一個七核Mn簇合物[MnⅡ3MnⅢ4(Cl)6(hmp)6(thme)2]· H2O·3CH3CN(1·H2O·3CH3CN，hmpH為2-吡啶甲醇，thmeH3為三羥甲基乙烷)，并對該化合物進行X射線衍射單晶結構分析、元素分析、紅外光譜和磁性研究。1·H2O·3CH3CN屬于單斜晶系I2/a空間群，配合物核骨架可看成由交替的MnⅡ和MnⅢ離子形成一個六邊形，而這個六邊形又圍繞在1個MnⅢ離子的周圍，這種結構類型的配合物以前并沒有報道過。磁性研究表明，化合物1·H2O中MnⅢ與MnⅡ或MnⅢ與MnⅢ離子之間總體是鐵磁性耦合的，交流磁化率研究發現該化合物有弱的頻率依賴現象。

七核Mn配合物；混合螯合配體；多齒螯合配體；晶體結構；磁性質

Since the discovery of slow magnetization relaxation for[Mn12O12(O2CMe)16(H2O)4]in 1993,single molecule magnets(SMMs)have received great attention in the field of coordination chemistry because of their unique and intriguing properties and their potential applications in high-density information storage, quantum computing and molecular spintronics[1-2].Up to date,polynuclear 3d transition metal complexes (especially polynuclear Mn clusters)[3-4],3d-4f mixedmetal complexes[5-6],polynuclear pure lanthanideclusters[7]and mononuclear f-based(including acitinide) or 3d transition metal compounds[8-10]have been reported by scientists all over the world.Nonetheless,we consider that the polynuclear 3d clusters,especially polynuclear Mn clusters,should not be ignored because it is important for better understanding of magnetic interactions between paramagnetic ions,the quantum tunneling of the magnetization and the mechanisms for slow magnetic relaxation.

Choosing appropriate multidentate chelating ligands is vitally important for obtaining the above types of SMMs.At early stage,carboxylate ligands have been widely used in the construction of 3d clusters. However,in recently years,non-carboxylate ligands have been received more attention.These non-carboxylate ligands mainly include[11]:(Ⅱ)alcohol/alkoxide -based chelating ligands,such as 2-(hydroxymethyl) pyridine(hmpH)[12],2,6-pyridinedimethanol(pdmH2)[13], the gem-diolate form of di-2-pyridyl ketone(dpkd2-)[14], 1,1,1-tris(hydroxymethyl)ethane(thmeH3)[15];(Ⅱ)polydentate Schiff-base ligands,such as N,N′-2,2-dimethylpropylenedi(3-methoxysalicylideneiminato)[16],(E)-2, 2′-(2-hydroxy-3-((2-hydroxyphenylimino)methyl)-5-methylbenzylazanediyl)-diethanol[17];(Ⅱ)other N-and O-based chelating ligands,such as methyl-2-pyridyl ketone(mpkoH)[18],2,6-diacetylpyridine dioxime (dapdoH2)[19],salicylaldoxime and its derivatives(H2salox and R-H2salox)[20].By detailed investigation on these multidentate chelating ligands,we found that their symmetry are different,for example,pdmH2and thmeH3possess C2and C3symmetry axes,respectively, while hmpH,mpkoH and others have no symmetry axes.Additionally,the coordinate modes of these multidentate chelating ligands are different from each other.Therefore,novel structural complexes with distinctive magnetic properties compared with complexes containing single multidentate chelating ligand may be obtained by mixing two or more kinds of ligands possessing different symmetry in a solution containing magnetic spin carrier salts.Actually,we have obtained[Mn4],[Mn13]and[Mn16]clusters containing mixed chelating ligands[21-22].We have also found that the core structures of the tetranuclear Ni clusters can be transformed from a defect dicubanelike core to a cubane-like core by adding of auxiliary multidentate chelating ligand of 2-(hydroxymethyl) pyridine ligands[23].As a part of our continuing studies on the synthesis and magnetic properties of SMMs clusters containing mixed multidentate chelating ligands,we report herein a heptanuclear Mn cluster, namely[MnⅡ3MnⅢ4(Cl)6(hmp)6(thme)2]·H2O·3CH3CN (1·H2O·3CH3CN).Magnetic studies reveal that overall ferromagnetic coupling betweenMnⅢand MnⅡor MnⅢions within complex 1·H2O are present and weak frequency dependence of the ac-susceptibility was found.

1　Experimental

1.1M aterials and measurements

All the starting materials for synthesis were commercially available and used as received. Elemental analyses for C,H and N were carried out using an Elementar Vario Perkin-Elmer 240C analyzer. IR spectra were obtained at room temperature using KBr pellets in the range of 4 000～400 cm-1on a VECTOR 22 spectrometer.Magnetic measurements on crystalline samples were performed on a Quantum Design MPMS-XL7 superconducting quantum interference device(SQUID)magnetometer.The direct current(dc)measurements were collected at an applied field of 2 kOe and from 1.8 to 300 K,and the alternating-current(ac)measurements were carried out in a 5.0 Oe ac field oscillating at various frequencies from 1 to 1 500 Hz and without dc field.The diamagnetic corrections for the compounds were estimated using Pascal′s constants,and magnetic data were corrected for diamagnetic contributions of the sample holder.

1.2Preparation of[M nⅡ3M nⅢ4(Cl)6(hmp)6(thme)2] ·H2O·3CH3CN(1·H2O·3CH3CN)

A mixture of MnCl2·4H2O(0.082 5 g,0.4 mmol), 1,1,1-tris(hydroxymethyl)ethane(0.049 4 g,0.4 mmol), 2-pyridinemethanol(0.045 5 g,0.4 mmol),triethylamine(0.126 g,1.2 mmol)in a molar ratio of 2∶1∶2∶2∶6 in CH3CN was stirred at room temperature for half an hour,forming a red-orange solution from which browncrystals of the compounds 1·H2O·3CH3CN were formed after several days.Yield:0.032 5 g(38%based on Mn).It should be noted that,for complex 1·H2O· 3CH3CN,vacuum-drying has resulted in three MeCN solvent molecules free.Anal.Calcd.for 1·H2O(C46H56Cl6Mn7N6O13,%):C,36.88;H,3.77;N,5.61.Found (%):C,36.78;H,3.68;N,5.57.IR(KBr,cm-1):3 422 (s),2 872(m),1 605(m),1 522(m),1 460(m),1 384 (m),1 122(w),1 047(s),915(w),763(w),582(m).

1.3X-ray crystallography

For compound 1·H2O·3CH3CN,the framework of single crystal samples was collapsed in the air a few minutes later,so the suitable single crystal of 1·H2O· 3CH3CN was located in a silica tube to collect crystallographic data.Diffraction data were collected on a Bruker Smart CCD area-detector diffractometer with Mo Kα radiation(λ=0.071 073 nm)by ω-scan mode operating at room temperature.The collected data were reduced with SAINT[24],and semi-empirical absorption correction was applied to the intensity data using the SADABS program[25].The structure was solved by direct methods,and all non hydrogen atoms were refined anisotropically by least squares on F2using the SHELXTL program[26].Hydrogen atoms were placed in calculated positions and refined isotropically using the riding model.Unit cell data and structure refinement details are listed in Table 1.

CCDC:1045766.

Table 1 Details of the data collection and refinement parameters for 1·H2O·3CH3CN

2　Results and discussion

2.1Crystal structure description

Single-crystal X-ray diffraction analysis revealed that complex 1·H2O·3CH3CN crystallizes in monoclinic space group I2/a.The crystal structure of complex 1·H2O·3CH3CN is shown in Fig.1.Selected bond lengths and angles are given in Table 2.As can be seen from Fig.1,complex 1·H2O·3CH3CN has seven manganese atoms that are roughly in the same plane. It consists of a central MnⅢion which is encircled by six Mn ions that form a roughly dislike heptanuclear Mn clusters.The outer six Mn atoms are connected with the central Mn through six μ3-O atoms(O7,O8, O9 and O10,O11,O12)which are from thme3-ligands located above and below the molecular plane, respectively.As can be seen from Fig.1,1·H2O· 3CH3CN contains six hmp-ligands,two thme3-ligands and six Cl-terminal ligands.Each of the hmp-ligands simultaneously binds two Mn atoms in a μ2-η1∶η2fashion.Each hydroxyl O from thme3-coordinates with three Mn ions,and the thme3-ligand binds seven Mn ions in a η3∶η3∶η3,μ7-fashion.Oxidation-state determinations based on charge considerations and crystallographic evidences for Jahn-Teller elongated axes.It is concluded that Mn1,Mn3,Mn5,Mn7 are MnⅢ, Mn2,Mn4,Mn6 are MnⅡ.All the Mn atoms are sixcoordinated with distorted octahedral geometry.For four MnⅢions,each of them clearly possesses a Jahn-Teller distortion in the form of axis elongation along N2-Mn1-O7,N3-Mn3-O10,N5-Mn5-O12 and O8-Mn7-O11(black lines in Fig.2),in which Jahn-Telleraxes for Mn1,Mn3 Mn7 are roughly parallel while these are vertical to that of Mn5.Besides,the O-Mn7-O is almost linear,with O11-Mn7-O8,O12-Mn7-O7 and O9-Mn7-O10 being 175.780°,177.41°and176.32°,respectively.For Mn2,Mn4 and Mn6 ions, the bond lengths of Mn-O and Mn-Cl are in the range of 0.208 3～0.287 7 nm(Mn4-O12 0.267 4 nm,Mn6-O9 0.287 7 nm)and 0.238 4～0.243 9 nm,respectively, which meet the feature of MnⅡions[27].

Fig.1 Molecular structure of comp lex 1·H2O·3CH3CN

Fig.2 Black lines showing Jahn-Teller axes of MnⅢions in the comp lex 1·H2O·3CH3CN

Table 2 Selected bond lengths(nm)and bond angles(°)for 1·H2O·3CH3CN

2.2M agnetic properties

The direct-current(dc)magnetic susceptibility measurements for polycrystalline samples of 1·H2O were performed between 1.8 and 300 K under an applied dc field of 2 000 Oe.The χMT versus T plot for 1·H2O was shown in Fig.3.At room temperature, the χMT value is 26.07 cm3·K·mol-1,which is slightly higher than the spin-only values of 25.13 cm3·K·mol-1expected for three MnⅡand four MnⅢnon-interacting ions.As the temperature is reduced to 30 K,the χMT product steadily increases to 32.46 cm3·K·mol-1and then drops to a value of 16.12 cm3·K·mol-1at 1.8 K. The χMvalues above 50 K obey the Curie-Weiss law (χM=C/(T-θ))with C=24.99 cm3·K·mol-1and θ=13.65 K.The positive θ value and the increase in χMT on lowering the temperature show that the overall ferromagnetic coupling interactions between Mn ions within the cluster are present.

Fig.3 Temperature dependence of χMT for 1·H2O

To obtain the sign and magnitude of the magnetic exchange interactions between Mn ions within the molecule of 1·H2O,fitting of the magnetic susceptibility data was carried out.Due to no symmetry in the complex,each distance between MnⅡ/MnⅢand MnⅢis different,so a precise fitting of the magnetic data require too many exchange constants.However,from the crystal structure,the alternative MnⅡand MnⅢatoms in the Mn6ring are linked by one hydroxyl group O atom of an hmp-and one O atom of a thme3-, and each of MnⅡor MnⅢin the Mn6ring is connected to the central Mn7 by two O atoms of two different thme3-ligands.Therefore,it is instructive to employ a simplified three-J model(Fig.4),which leads to the following Heisenberg Hamiltonian:

Fig.4 Model for fitting the magnetic data of 1·H2O

It should be noted that the above Heisenberg Hamiltonian based on the magnetic isotropic parameters,due to the dimension of full energy matrix being 135 000 for[MnⅡ3MnⅢ4]if the magnetic anisotropic parameters were employed,which goes beyond the operating limit of our computer.The magnetic data above 30 K have been fitted by MAGPACK program[28], with the best parameters being:J1=-0.6 cm-1,J2= 4.1 cm-1,J3=0.75 cm-1,g=2.0 and R=4.15×10-4(R=∑[(χMT)obs-(χMT)calc]2/∑(χMT)obs2).The signs of the coupling constants show that the antiferromagnetically coupling interactions are present in the Mn6ring,in which MnⅡand MnⅢare further antiferromagnetically and ferromagnetically coupled to the central MnⅢion, respectively.

To obtain the ground-state S,g and the magnitude of the zero-field splitting(ZFS)parameter(D),magnetization data were collected in the range of 1～7 T and 1.8～5.0 K.The plot of the reduced magnetization Mversus H/T shows that the curves are not superposed (Fig.5),giving an indication of the presence of magnetic anisotropy and/or the low-lying excited states.The magnetization data were fitted using the program ANISOFIT 2.0[29],by matrix diagonalization to a model with axial ZFS(DSz2)and isotropic Zeeman interactions,assuming only the ground state is populated.However,an acceptable fit could not be obtained using the data collected over the whole field range.This problem widely exits in high-nuclear clusters containing Mn2+ions[30],which is caused by low-lying excited states,especially if some have an S value greater than that of the ground state(in other words,these excited states are populated even at low temperatures and at low magnetic fields).This conclusion is supported by the M versus H plot(Fig. 6),in which the magnetization steadily increases upon increasing magnetic field(H)and does not show saturation.

Fig.5 Plots of reduced magnetization M vs H/T for 1·H2O

Fig.6 Plots of magnetization M vs H for 1·H2O

To probe the magnetization relaxation dynamics of 1·H2O,alternating current(ac)magnetic susceptibility data were collected in a zero-applied dc field with a 5.0 Oe ac field oscillating at frequencies in the range of 1～1488 Hz and in the temperature range of 1.8～10 K.The in-phase(χ′M,plotted as χ′MT)and outof-phase(χ″M)ac susceptibility signals are shown in Fig.7.The rapid decrease of χ′MT with temperatures decreasing also supports a population of low-lying excited states with larger S compared to the groundstate S.Extrapolation of χ′MT data down to 0 K gives～22.5 cm3·K·mol-1[31],obtaining a ground state of S≈6.5(Fig.8).At lower temperatures(below 2.8 K),the frequency-dependent χ″Msignals appear(Fig.7),indicating slow relaxation of the SMMs behavior. However,the peak maxima may lie at temperature below 1.8 K,which goes beyond the operating limit of our instrument.Therefore,we cannot calculate the effective energy barrier(Ueff)by the Arrhenius law.

Fig.7 Plot of the temperature dependence of the out-ofphase(χ″M)ac susceptibility signals for 1·H2O at the indicated frequencies

Fig.8χ′MT vs T plot for 1·H2O

2.3Compared with other[M n7]clusters

It should be noted that,in the literature,there are 14 reported dislike heptanuclear Mn clusters[32], which can be classified into four categories according to their oxidation states and their distribution of the Mn ions.The first class is MnⅡ4MnⅢ3,in which alternating MnⅡand MnⅢions consist of a six-member ring(Mn6ring)that encircles the central MnⅡions. The distribution of Mn ions of the second series MnⅡ7and the third class MnⅢ6MnⅡ(only one compound was reported),are the same as the above class,except all MnⅢfor the former series replaced by MnⅡions and MnⅡions on the Mn6ring for the later class replaced by MnⅢion,respectively.However,for the last category MnⅡ3MnⅢ4,the distribution of Mn ions is entirely different from the above three class,in this category, three MnⅡions consist of a linear,with its either side located by two MnⅢions.For 1·H2O·3CH3CN, alternating MnⅡand MnⅢions form a Mn6ring that encircles the central MnⅢ,which is similar to that of the first class mentioned above,except the different oxidation state of the central Mn.Therefore,complex 1·H2O·3CH3CN represents an unprecedented oxidation state configuration,which has previously not been seen for this topology.For 1·H2O·3CH3CN,the central Mn is coordinated to six O atoms from two thme3-ligands,so the change of central Mn compared to the first class may be due to the charge considerations and constraints imposed by multidentate chelating ligand thme3-.Therefore,this paper provides a chance for changing structural configuration and/or oxidation state of polynuclear magnetic clusters by mixing two or more multidentate chelating ligands with different symmetry.Finally,it also should be noted that only a few of dislike heptanuclear Mn clusters show SMMs behaviors and 1·H2O·3CH3CN showing this magnetic behavior may be due to the very subtle changes of oxidation state of the central Mn.

3　Conclusions

In summary,a complex containing mixed multidentate chelating ligands with different symmetry,i.e.[MnⅡ3MnⅢ4(Cl)6(hmp)6(thme)2]·H2O· 3CH3CN(1·H2O·3CH3CN),has been synthesized by the reactions of MnCl2·4H2O,hmpH and thmeH3in MeCN.For 1·H2O·3CH3CN,alternating MnⅡand MnⅢions form a Mn6ring that encircles the central MnⅢ, and this structural topology has previously not been seen.This structural change may be due to the charge considerations and constraints imposed by multidentate chelating ligand thme3-.Magnetic studies reveal that the overall ferromagnetic interactions between neighboring Mn atoms within 1·H2O are present,and weak frequency dependence of the ac-susceptibility was found,which represents a few of examples with SMMs behavior in dislike Mn7clusters.Finally,this work provides a chance for changing structural configuration and/or oxidation state of polynuclear magnetic clusters by mixing two or more multidentate chelating ligands with different symmetry.

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Synthesis,Crystal Structure and M agnetic Properties of a Heptanuclear M n Com p lex w ith 2-(Hydroxymethyl)pyridine and 1,1,1-Tris(hydroxymethyl)ethane M ixed-Ligands

WANG Hui-Sheng＊YUE Lin PAN Min ZHONG Wen-Da TU Wei PAN Zhi-Quan＊
(School of Chemistry and Environmental Engineering,Wuhan Institute of Technology,Key Laboratory for Green Chemical Process of Ministry of Education,Wuhan 430074,China)

One heptanuclear Mn cluster[MnⅡ3MnⅢ4(Cl)6(hmp)6(thme)2]·H2O·3CH3CN(1·H2O·3CH3CN,hmpH=2-(hydroxymethyl)pyridine and thmeH3=1,1,1-tris(hydroxymethyl)ethane)has been synthesized by the reaction of MnCl2·4H2O,hmpH and thmeH3in MeCN.The complex was characterized by single crystal X-ray diffraction, elemental analyses,IR and magnetic investigation.Complex 1·H2O·3CH3CN crystallizes in the monoclinic space group I2/a and its core can be viewed as a Mn6hexagon of alternating MnⅡand MnⅢions surrounding a central MnⅢion,which has previously not been seen for this topology.Magnetic studies reveal that overall ferromagnetic coupling between MnⅢand MnⅡor MnⅢions within 1·H2O are present and weak frequency dependence of the ac-susceptibility was found.CCDC:1045766.

heptanuclear Mn complex;mixed-chelating ligand;multidentate chelating ligand;crystal structure;magnetic property

O614.71+1

A

1001-4861(2016)01-0153-08

10.11862/CJIC.2016.012

2015-09-02。收修改稿日期：2015-11-04。

國家自然科學基金(No.21201136)和武漢工程大學科學研究基金(No.K201447)資助項目。

＊通信聯系人。E-mail：wangch198201@163.com，zhiqpan@163.com；會員登記號：S06N3619M1308。