The structure of Ba2Ni(PO4)2 was solved by single crystal X-ray diffraction. It crystallizes in the monoclinic system with the space group P2(1)/n. The cell parameters are a = 5.312(1) angstrom, b = 8.789(2) angstrom, c = 16.067(3) angstrom and beta = 90.72(1)-degrees, Z = 4. The structure has been refined from 2979 independent reflections to R = 0.031 (Rw = 0.039). The three dimensional framework could be described from comer and edge-sharing NiO6 octahedra and PO4 tetrahedra creating two types of tunnels where are located the barium ions. Magnetic thermal susceptibility has been described in terms of antiferromagnetic isotropic interactions in dimers of Ni2+(S = 1). The best agreement between theoretical and experimental data is obtained for J = -3.93 K and g = 2. 1. The specific heat measurements suggest a second order phase transition to a magnetical 3D- order state at low temperature (T < 5.17K).
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Chinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R ChinaChinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R China
He, Zhangzhen
Zhang, Weilong
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Chinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R ChinaChinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R China
Zhang, Weilong
Xia, Tianlong
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Renmin Univ China, Dept Phys, Beijing 100872, Peoples R ChinaChinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R China
Xia, Tianlong
Yu, Weiqiang
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Renmin Univ China, Dept Phys, Beijing 100872, Peoples R ChinaChinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R China
Yu, Weiqiang
Cheng, Wendan
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Chinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R ChinaChinese Acad Sci, State Key Lab Struct Chem, Fujian Inst Res Struct Mater, Fuzhou 350002, Fujian, Peoples R China
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Tata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, IndiaTata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, India
Yogi, Arvind
Bera, A. K.
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Bhabha Atom Res Ctr, Div Solid State Phys, Bombay 400005, Maharashtra, IndiaTata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, India
Bera, A. K.
Maurya, Arvind
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Tata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, IndiaTata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, India
Maurya, Arvind
Kulkarni, Ruta
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Tata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, IndiaTata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, India
Kulkarni, Ruta
Yusuf, S. M.
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Bhabha Atom Res Ctr, Div Solid State Phys, Bombay 400005, Maharashtra, IndiaTata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, India
Yusuf, S. M.
Hoser, A.
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Helmholtz Zentrum Berlin Mat & Energie, D-14109 Berlin, GermanyTata Inst Fundamental Res, Dept Condensed Matter Phys & Mat Sci, Homi Bhabha Rd, Bombay 400005, Maharashtra, India