Magnetic ground state and phase diagram, Hc(T), for magnetically ordered [Ru2(O2CMe)4]3[Cr(CN)6]
被引:30
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作者:
Shum, William W.
论文数: 0引用数: 0
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机构:
Univ Utah, Dept Chem, Salt Lake City, UT 84112 USAUniv Utah, Dept Chem, Salt Lake City, UT 84112 USA
Shum, William W.
[1
]
Schaller, Jason N.
论文数: 0引用数: 0
h-index: 0
机构:
Univ Utah, Dept Chem, Salt Lake City, UT 84112 USAUniv Utah, Dept Chem, Salt Lake City, UT 84112 USA
Schaller, Jason N.
[1
]
Miller, Joel S.
论文数: 0引用数: 0
h-index: 0
机构:
Univ Utah, Dept Chem, Salt Lake City, UT 84112 USAUniv Utah, Dept Chem, Salt Lake City, UT 84112 USA
Miller, Joel S.
[1
]
机构:
[1] Univ Utah, Dept Chem, Salt Lake City, UT 84112 USA
来源:
JOURNAL OF PHYSICAL CHEMISTRY C
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2008年
/
112卷
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21期
关键词:
D O I:
10.1021/jp711835f
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 magnetic phase diagram for [Ru-2(O2CMe)(4)](3)[Cr(CN)(6)] was determined from temperature dependent isothermal magnetization studies below its 33-K T-c. Below similar to 25 K, the change in slope of the M(H) for similar to 1100 +/- 400 Oe increases with increasing temperature, as does the initial slope at lower applied field, whereas above similar to 25 K, the slope decreases with increasing temperature. The M(H) below its 25-K tricritical point is characteristic of a first order transition, whereas above 25 K, it is characteristic of a second order transition. The magnetic phase diagram of [Ru-2(O2CMe)(4)](3)[Cr(CN)(6)] is characteristic of a class I metamagnet and has an antiferromagnetic ground-state arising from antiferromagnetically coupled ferrimagnetic lattices.