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rubidium manganese hexacyanoferrate | 412009-41-7

中文名称
——
中文别名
——
英文名称
rubidium manganese hexacyanoferrate
英文别名
rubidium(I) manganese(II) hexacyanoferrate(III);Iron(3+);manganese(2+);rubidium(1+);hexacyanide
rubidium manganese hexacyanoferrate化学式
CAS
412009-41-7
化学式
C6FeN6*Mn*Rb
mdl
——
分子量
352.359
InChiKey
GMPNLNQUZXHGIP-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):
    -2.42
  • 重原子数:
    15
  • 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:
    143
  • 氢给体数:
    0
  • 氢受体数:
    12

反应信息

  • 作为反应物:
    描述:
    rubidium manganese hexacyanoferrate 以 neat (no solvent, solid phase) 为溶剂, 生成 RbMn(Fe(CN)6), cubic, high temperature
    参考文献:
    名称:
    Extended Charge-Transfer State of RbMn[Fe(CN)6]
    摘要:
    Based on the maximum entropy method (MEM) charge density, we have visualized the electrostatic potential of a charge-transfer compound, RbMn[Fe(CN)6], which shows the charge-transfer transition from the nominal Mn2+-Fe3+ configuration to the Mn3+-Fe2+ one below 220 K. In the low-temperature phase, the transferred electron spreads over the hexacyanoferrate ([Fe(CN)61) via the strong Fet(2g)-CN pi* hybridization. Such an extended charge-transfer state is responsible for the relatively strong ferromagnetic coupling between the neighbouring Mn3+ spins.
    DOI:
    10.1143/jpsj.76.123602
  • 作为产物:
    描述:
    rubidium chloride 、 manganese(ll) chloride 、 potassium hexacyanoferrate(III) 以 为溶剂, 生成 rubidium manganese hexacyanoferrate
    参考文献:
    名称:
    铁磁态和顺磁态下铷锰六氰基铁酸盐的光致电荷转移相变
    摘要:
    摘要 在一系列铷锰六氰基铁酸盐 RbMn[Fe(CN) 6 ] ( 1 ), Rb 0.88 Mn[Fe(CN) 6 ] 0.96 ·0.6H 2 O ( 2 ) 中观察到了具有热滞回线的电荷转移相变),Rb 0.97 Mn[Fe(CN) 6 ] 0.99 ·0.2H 2 O ( 3 )。这种相变伴随着从立方(F4¯3m)到四方(I4¯m2)的结构变化。其高温 (HT) 和低温 (LT) 相由 Mn II ( S = 2 / 5 ) NC – Fe III ( S = 1 / 2 ) 和 Mn III ( S = 2 ) – NC – Fe 组成II ( S = 0 ) ,分别。相变是由金属到金属的电荷从 Mn II 转移到 Fe III 以及产生的 Mn III 离子的 Jahn-Teller 畸变引起的。在 LT 相的铁磁状态为 2 时,观察到光致相变,即仅用一束激光脉冲照射就淬灭了磁化强度。这种现象是由从
    DOI:
    10.1016/j.jmmm.2006.10.429
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文献信息

  • Structural Transition Induced by Charge-Transfer in RbMn[Fe(CN)<sub>6</sub>] –Investigation by Synchrotron-Radiation X-ray Powder Analysis–
    作者:Yutaka Moritomo、Kenichi Kato、Akira Kuriki、Masaki Takata、Makoto Sakata、Hiroko Tokoro、Shin-ichi Ohkoshi、Kazuhito Hashimoto
    DOI:10.1143/jpsj.71.2078
    日期:2002.9
    determined for RbMn[Fe(CN) 6 ] by means of synchrotron-radiation (SR) X-ray powder structural analysis. We observed a structural transition from the cubic (F\(\overline4}\)3m; Z = 4) to the tetragonal (I\(\overline4}\)m2; Z = 2) phase at ≈ 210 K in the cooling run and at ≈ 300 K in the warming run. In the low-temperature tetragonal phase, we found Jahn–Tellar type distortion of the MnN 6 octahedra and compression
    通过同步辐射 (SR) X 射线粉末结构分析,确定 RbMn[Fe(CN) 6 ] 原子坐标的温度依赖性。我们在 ≈ 210 K 观察到从立方 (F\(\overline4}\)3m; Z = 4) 到四方 (I\(\overline4}\)m2; Z = 2) 相的结构转变在冷却运行中和在升温运行中 ≈ 300 K。在低温四方相中,我们发现 MnN 6 八面体的 Jahn-Tellar 型畸变和平均 Fe-C 键距的压缩。这些结构数据表明结构转变是由从 Mn(II) 位点到 Fe(III) 位点的属间电荷转移触发的。
  • A Large Thermal Hysteresis Loop Produced by a Charge-Transfer Phase Transition in a Rubidium Manganese Hexacyanoferrate
    作者:Hiroko Tokoro、Shin-ichi Ohkoshi、Tomoyuki Matsuda、Kazuhito Hashimoto
    DOI:10.1021/ic030332f
    日期:2004.8.1
    In a rubidium manganese hexacyanoferrate, RbMn[Fe(CN)(6)], the magnetic susceptibility (chi(M)) decreased at 225 K (=T(1/2)decreasing) and abruptly increased at 300 K (=T(1/2)increasing) in the cooling and warming processes, respectively. X-ray photoelectron spectroscopy and infrared spectroscopy indicated that the high-temperature (HT) and low-temperature (LT) phases were composed of Mn(II)-NC-Fe(III)
    在六man RbMn [Fe(CN)(6)]中,磁化率(chi(M))在225 K(= T(1/2)减小)时降低,而在300 K(= T(在冷却和加热过程中分别增加1/2)。X射线光电子能谱和红外光谱表明,高温(HT)和低温(LT)相由Mn(II)-NC-Fe(III)和Mn(III)-NC-Fe(II)组成), 分别。从立方(F43m,a = 10.533 A)到四方形(I4m2,a = b = 7.090 A,c = 10.520 A)的结构变化伴随相变而变化,根据这些结果,HT和LT相为分配给Mn(II)(t(2g)(3)e(g)(2),(6)A(1g); S =(5)/(2))-NC-Fe(III)(t( 2g)(5),(2)T(2g); S =(1)/(2))和Mn(III)(e(g)(2)b(2g)(1)a(1g)(1 ),(5)B(1g); S = 2)-NC-Fe
  • Mössbauer investigation of the thermal phase transition in RbMnFe(CN)6
    作者:He Yun、Tang Guodong、Liang Fupei、Huang Yanjun、Huang Mali
    DOI:10.1016/j.jallcom.2006.08.039
    日期:2007.7
    Abstract One of the Prussian blue analogs, RbMnFe(CN) 6 , was investigated by Mossbauer spectroscopy in the cooling and warming processes. The thermal phase transition was testified by Mossbauer studies. The high-temperature (HT) phase and low-temperature (LT) phase could be respectively determined to be Mn 2+ ( S = 5/2)–NC–Fe 3+ ( S = 1/2) and Mn 3+ ( S = 2)–NC–Fe 2+ ( S = 0).
    摘要 在冷却和升温过程中,通过穆斯堡尔光谱研究了一种普鲁士蓝类似物 RbMnFe(CN) 6 。Mossbauer 研究证实了热相变。高温 (HT) 相和低温 (LT) 相可以分别确定为 Mn 2+ ( S = 5/2)–NC–Fe 3+ ( S = 1/2) 和 Mn 3+ ( S = 2)–NC–Fe 2+ ( S = 0)。
  • Observation of Spin Transition in an Octahedrally Coordinated Manganese(II) Compound
    作者:Shin-ichi Ohkoshi、Hiroko Tokoro、Masayoshi Utsunomiya、Mikihisa Mizuno、Masahiko Abe、Kazuhito Hashimoto
    DOI:10.1021/jp0133687
    日期:2002.3.1
    The thermal spin transition between a high-spin state (S = 5/2) and an intermediate-spin state (S = 3/2) of the octhahedrally coordinated Mn(II)(3d(5)) was observed in Rb(I)Mn(II)[Fe(III)(CN)(6)] with a very wide hysteresis loop over the temperature range of 231 to 304 K. This phenomenon is accompanied by a structural distortion from the face-centered cubic structure to the tetragonal one caused by a cooperative Jahn-Teller effect in the octahedral Fe(III)C-6 moiety. To our knowledge, the present spin transition is the first observation in compounds containing a six-coordinated Mn(II).
  • Ferromagnetic Spin-Ordering in Photo-active RbMn[Fe(CN)<sub>6</sub>]
    作者:Yutaka Moritomo、Akira Kuriki、Kenji Ohoyama、Hiroko Tokoro、Shin-ichi Ohkoshi、Kazuhito Hashimoto、Noriaki Hamada
    DOI:10.1143/jpsj.72.456
    日期:2003.2.15
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