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Manganese--platinum (3/1) | 12163-58-5

中文名称
——
中文别名
——
英文名称
Manganese--platinum (3/1)
英文别名
manganese;platinum
Manganese--platinum (3/1)化学式
CAS
12163-58-5
化学式
Mn3Pt
mdl
——
分子量
359.894
InChiKey
QSGMISIZWMTPQR-UHFFFAOYSA-N
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    -0.01
  • 重原子数:
    4
  • 可旋转键数:
    0
  • 环数:
    0.0
  • sp3杂化的碳原子比例:
    0.0
  • 拓扑面积:
    0
  • 氢给体数:
    0
  • 氢受体数:
    0

反应信息

  • 作为产物:
    描述:
    以 neat (no solvent) 为溶剂, 生成 Manganese--platinum (3/1)
    参考文献:
    名称:
    Spin Fluctuations in an Octahedral Antiferromagnet Mn3Pt Alloy
    摘要:
    A new spin frustration system with an octahedral configuration of magnetic atoms was found. In neutron scattering measurements for an ordered Mn3Pt alloy, inelastic diffuse scattering intensity distributes along the first Brillouin zone-boundary of the fee structure in the paramagnetic and the F-phases. Within the calculations based on a RPA, the experimental data in the paramagnetic phase are reproduced using antiferromagnetic couplings between the spins up to the third-neighbor exchange interactions. In the F-phase below the Neel temperature, a part of the Mn spins still fluctuates at the special site. The existence of the F-phase is a characteristic of the octahedral spin frustration system. The effects of the chemical disorder on the spin frustration are also studied using a specimen with a small atomic LRO parameter.
    DOI:
    10.1143/jpsj.72.2614
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文献信息

  • Spin Fluctuations in an Octahedral Antiferromagnet Mn<sub>3</sub>Pt Alloy
    作者:Takashi Ikeda、Yorihiko Tsunoda
    DOI:10.1143/jpsj.72.2614
    日期:2003.10.15
    A new spin frustration system with an octahedral configuration of magnetic atoms was found. In neutron scattering measurements for an ordered Mn3Pt alloy, inelastic diffuse scattering intensity distributes along the first Brillouin zone-boundary of the fee structure in the paramagnetic and the F-phases. Within the calculations based on a RPA, the experimental data in the paramagnetic phase are reproduced using antiferromagnetic couplings between the spins up to the third-neighbor exchange interactions. In the F-phase below the Neel temperature, a part of the Mn spins still fluctuates at the special site. The existence of the F-phase is a characteristic of the octahedral spin frustration system. The effects of the chemical disorder on the spin frustration are also studied using a specimen with a small atomic LRO parameter.
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