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Fabrication and magnetic properties of 4SC(NH_2)_2–Ni_(0.97)Cu_(0.03)Cl_2 single crystals
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作者 陈丽敏 郭颖 +5 位作者 刘旭光 解其云 陶志阔 谌静 周玲玲 刘春生 《Chinese Physics B》 SCIE EI CAS CSCD 2015年第12期541-544,共4页
Single crystals of 4SC(NH2)2–Ni1-xCux Cl2(x = 0.03)(Cu-DTN) containing spin S = 1/2 Cu^2+and S = 1 Ni^2+cations are synthesized by slow evaporation methods. Structural characterization demonstrates that the C... Single crystals of 4SC(NH2)2–Ni1-xCux Cl2(x = 0.03)(Cu-DTN) containing spin S = 1/2 Cu^2+and S = 1 Ni^2+cations are synthesized by slow evaporation methods. Structural characterization demonstrates that the Cu-DTN is of a tetrahedral structure with lattice parameter c being 9.0995 A, which is 1.32% expansion compared with that of parent material DTN due to the larger radius of the Cu ion. Direct current(DC) susceptibility measurements show that both the antiferromagnetic exchange interaction at low temperature and the large anisotropy of susceptibilities are suppressed after doping the Cu ion, which could be related to the structural distortion and the increase of the super-exchange paths in Cu-DTN. 展开更多
关键词 magnetic metal-doped magnetic materials susceptibility antiferromagnetic interaction
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Chiral mesostructured hematite with temperature-independent magnetism due to spin confinement 被引量:1
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作者 Baiwen Zhang Jing Ai +3 位作者 Yingying Duan Te Bai Lu Han Shunai Che 《Nano Research》 SCIE EI CSCD 2024年第3期2019-2024,共6页
Hematite(α-Fe_(2)O_(3))is known to undergo conversion from weak ferromagnetic to antiferromagnetic as the temperature decreases below the Morin temperature(TM=250 K)due to spin moment rotation occurring during the Mo... Hematite(α-Fe_(2)O_(3))is known to undergo conversion from weak ferromagnetic to antiferromagnetic as the temperature decreases below the Morin temperature(TM=250 K)due to spin moment rotation occurring during the Morin transition(MT).Herein,we endowed hematite with mesostructured chirality to maintain weak ferromagnetism without MT.Chiral mesostructured hematite(CMH)nanoparticles were prepared by a hydrothermal method with glutamic acid(Glu)as the symmetry-breaking agent.The triangular bipyramidal CMH nanoparticles were composed of helically cleaved nanoflakes with twisted crystal lattice.Field-cooled(FC)magnetization measurements showed that the magnetic moments of CMH were stabilized without MT within the temperature range of 10–300 K.Hysteresis loop measurements confirmed the weak ferromagnetism of CMH.The enhanced Dzyaloshinskii–Moriya interaction(DMI)was speculated to be responsible for the temperature-independent weak ferromagnetism,in which the spin configuration would be confined with canted antiferromagnetic coupling due to the mesostructured chirality of CMH. 展开更多
关键词 HEMATITE chiral mesostructure Dzyaloshinskii–Moriya interaction weak ferromagnetism antiferromagnetic material temperature-independent magnetism
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SYNTHESIS, STRUCTURE AND MAGNETISM OF μ-OXAMIDO BINUCLEAR COPPER(Ⅱ) COMPLEXES
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作者 张智勇 廖代正 +4 位作者 姜宗慧 郝松棋 姚心侃 王宏根 王耕霖 《Science China Chemistry》 SCIE EI CAS 1991年第3期265-273,共9页
<正> Two new binuclear copper(Ⅱ) complexes, [Cu(oxpn)CuL](ClO4)2, have been synthesizedand characterized, where oxpn is N,N’ bis(3-aminopropyl)oxamido and L is 1,10-phenan-throline (phen) or 5-nitro-... <正> Two new binuclear copper(Ⅱ) complexes, [Cu(oxpn)CuL](ClO4)2, have been synthesizedand characterized, where oxpn is N,N’ bis(3-aminopropyl)oxamido and L is 1,10-phenan-throline (phen) or 5-nitro-1,10-phenanthroline (NO2-phen). The crystal structure and vari-able-temperature magnetic susceptibility (4- 300 K) of the Complex (L=phen) have beendetermined. Crystal data: orthorhombic system, space group Pnma, with a = 10.433(1), b11.458(2), c = 21.999(2)A, z = 4. Every copper(Ⅱ) ion is in a square pyramidal environment.The two copper(Ⅱ) ions are linked by μ-oxamido bridge and the separation of them is 5.208A. The singlet-triplet energy gap J was found equal to -452.92cm-1, indicating that astrongantiferromagnetic spin-exchange interaction operates between the copper(Ⅱ) ions. 展开更多
关键词 BINUCLEAR copper(Ⅱ) complex VARIABLE-TEMPERATURE magnetic susceptibility antiferromagnetic SPIN-EXCHANGE interaction
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