Experimental and Theoretical Characterization of the Magnetic Properties of CuF2(H2O)2(pyz) (pyz = pyrazine): A Two-Dimensional Quantum Magnet Arising from Supersuperexchange Interactions through Hydrogen Bonded Paths

被引:57
|
作者
Manson, Jamie L. [1 ]
Conner, Marianne M. [1 ]
Schlueter, John A. [2 ]
McConnell, Amber C. [1 ]
Southerland, Heather I. [1 ]
Malfant, Isabelle [3 ]
Lancaster, Tom [4 ]
Blundell, Stephen J. [4 ]
Brooks, Michael L. [4 ]
Pratt, Francis L. [5 ]
Singleton, John [6 ]
McDonald, Ross D. [6 ]
Lee, Changhoon [7 ]
Whangbo, Myung-Hwan [7 ]
机构
[1] Eastern Washington Univ, Dept Chem & Biochem, Cheney, WA 99004 USA
[2] Argonne Natl Lab, Div Mat Sci, Argonne, IL 60439 USA
[3] Maitre Conf Univ Paul Sabatier, CNRS, Chim Coordinat Lab, UPR 8241, F-31077 Toulouse, France
[4] Univ Oxford, Dept Phys, Clarendon Lab, Oxford OX1 3PU, England
[5] Rutherford Appleton Lab, ISIS Facil, Didcot OX11 0QX, Oxon, England
[6] Los Alamos Natl Lab, Natl High Magnet Field Lab, Los Alamos, NM 87545 USA
[7] N Carolina State Univ, Dept Chem, Raleigh, NC 27695 USA
基金
英国工程与自然科学研究理事会;
关键词
D O I
10.1021/cm8016566
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The structural. electronic, and magnetic properties of the new linear chain coordination polymer CuF2(H2O)(2)(pyz) (pyz = pyrazine) were determined by single crystal X-ray diffraction at various temperatures, SQUID magnetometry, pulsed-field magnetization, ESR, muon-spin relaxation (mu SR), and electronic structure calculations. Each Cu2+ ion of CuF2(H2O)(2)(pyz) is located at a distorted CuF2O2N2 octahedron with axial elonclation along the Cu-N bonds. These octahedra are tethered to-ether by strong F center dot center dot center dot H-O hydrogen bonds to yield two-dimensional (2D) square nets in the bc-plane that are linked alone, the a-direction by pyrazine linkages. Measurements of the g-factor by ESR along with first principles density functional theory electronic structure calculations show that the magnetic orbital of the Cu2+ ion lies in the CuF2O2 plane thus forming a 2D antiferromagnetic square lattice. A broad maximum observed in chi(T) at 10 K indicates a modest spin exchange interaction through the Cu-F center dot center dot center dot H-O-Cu supersuperexchange paths, and a theoretical fit of chi(T) to a 2D square model gives J(2D)/k(B) = -5.58(1) K (in the convention where J rather than 2J is used for spin exchange). At lower temperatures, chi(T) shows a sharp peak at similar to 2.6 K. which si-nals a transition to a lon-ran-e maonetic orderine, as confirmed by coherent precession of implanted muons. Isothermal M(B) measurements made at 0.5 K on an aligned single crystal reveal magnetic saturation, M-sat at 28.8 T (B parallel to a) while a higher field of 33.1 T is required to saturate the spins when B is applied perpendicular to the a-axis thus showing clear anisotropy in these orientations. The presence of strong hydrogen bonds in CuF2(H2O)(2)(pyz) causes the chains to adopt a tilted packing arrangement, thus leading to a novel ground-state likely characterized by spin-canting within the 2D layers and a markedly increased critical temperature relative to the well-known Cu(NO3)(2)(pyz) polymer chain compound.
引用
收藏
页码:7408 / 7416
页数:9
相关论文
共 50 条
  • [21] Synthesis, crystal structure and magnetic properties of [Mn(LH)2(H2O)2]n with a two-dimensional layered structure and three-dimensional hydrogen bonding network
    Qihua Zhao
    Haifang Li
    Ruibin Fang
    Transition Metal Chemistry, 2003, 28 : 220 - 223
  • [22] Synthesis, crystal structure and magnetic properties of [Mn(LH)2(H2O)2]n with a two-dimensional layered structure and three-dimensional hydrogen bonding network
    Zhao, QH
    Li, HF
    Fang, RB
    TRANSITION METAL CHEMISTRY, 2003, 28 (02) : 220 - 223
  • [23] 3D networks constructed using both coordinative and hydrogen bonding:: synthesis, structure and magnetic properties of M(tcm)2(H2O)2•Me4pyz, M = Co, Ni
    Batten, SR
    Hoskins, BF
    Moubaraki, B
    Murray, KS
    Robson, R
    CRYSTENGCOMM, 2001, (08):
  • [24] Experimental Study of the Magnetocaloric Effect in the Two-Dimensional Quantum System Cu(en)(H2O)2SO4
    Tarasenko, R.
    Sedlakova, L.
    Orendacova, A.
    Orendac, M.
    Feher, A.
    26TH INTERNATIONAL CONFERENCE ON LOW TEMPERATURE PHYSICS (LT26), PTS 1-5, 2012, 400
  • [25] Crystal Structure and Magnetic Properties of a Two-dimensional Compound {(Me2NH2)4[Co(SIP)2]•2(DMF)•3(H2O)}n
    Xiong Ling-Na
    Liu Qing-Yan
    Wang Yu-Ling
    CHINESE JOURNAL OF STRUCTURAL CHEMISTRY, 2016, 35 (08) : 1231 - 1237
  • [26] Crystal Structure and Magnetic Properties of a Two-dimensional Compound{(Me2NH2)4[Co(SIP)2]·2(DMF)·3(H2O)}n
    熊灵娜
    刘庆燕
    王玉玲
    结构化学, 2016, 35 (08) : 1231 - 1237
  • [27] Crystal structure and magnetic properties of manganese(II) mellitate, [Mn-2{C-6(COO)(6)}(H2O)(6)][Mn(H2O)(6)]center dot 2H(2)O with two-dimensional layered structure and three-dimensional hydrogen bonding networks
    Wu, LP
    Yamamoto, M
    KurodaSowa, T
    Maekawa, M
    Fukui, J
    Munakata, M
    INORGANICA CHIMICA ACTA, 1995, 239 (1-2) : 165 - 169
  • [28] Structure and magnetic properties of a two-dimensional layered manganese(II) pyrophosphate [NH4]2[Mn3(P2O7)2(H2O)2]
    Shi, L
    Yu, JH
    Li, Y
    Xu, RR
    Gao, S
    CHINESE JOURNAL OF INORGANIC CHEMISTRY, 2005, 21 (02) : 245 - 248
  • [29] Structure and magnetic properties of a novel two-dimensional complex from 1,3,5-benzenetricarboxylate and neodymium(III) -: {[Nd(1,3,5-benzenetricarboxylate)(H2O)4]•H2O}n
    Wang, QL
    Liang, M
    Liao, DZ
    Yan, SP
    Jiang, ZH
    Cheng, P
    ZEITSCHRIFT FUR ANORGANISCHE UND ALLGEMEINE CHEMIE, 2004, 630 (04): : 613 - 616
  • [30] Synthesis, crystal structure and magnetic properties of Ni3(H2O)6(TMA)3-(TMA)23-•2H2O with two-dimensional aperture strucutre
    Chen, W
    Tan, XN
    Li, YM
    Zheng, JM
    Che, YX
    CHINESE JOURNAL OF INORGANIC CHEMISTRY, 2005, 21 (12) : 1901 - 1904