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首页> 外文期刊>Dalton transactions: An international journal of inorganic chemistry >Charge-transfer phase transition and zero thermal expansion in caesium manganese hexacyanoferrates
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Charge-transfer phase transition and zero thermal expansion in caesium manganese hexacyanoferrates

机译:六价高铁酸铯锰中的电荷转移相变和零热膨胀

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A series of caesium manganese hexacyanoferrates is prepared; (Cs1.78MnII)-Mn-I[Fe-II(CN)(6)](0.78)[Fe-III(CN)(6)](0.22) ( 1), Cs-I Mn-1.57(II)[Fe-II(CN)(6)](0.57)[Fe-III(CN)(6)](0.43) ( 2), Cs-I Mn-1.51(II)[Fe-II(CN)(6)](0.51)[Fe-III(CN)(6)](0.49) (3), and Cs-I Mn-0.94(II)[Fe-II(CN)(6)](0.21)[Fe-III(CN)(6)](0.70) center dot 0.8H(2)O ( 4). 1 - 3 show charge-transfer phase transitions between the high-temperature (HT) and low-temperature (LT) phases with transition temperatures (T-1/2 down arrow, T-1/2 up arrow) of ( 207 K, 225 K) ( 1), ( 190 K, 231 K) ( 2), and ( 175 K, 233 K) ( 3) at a cooling and warming rates of 0.5 K min(-1). Variable temperature IR spectra indicate that the valence states of the LT phases of 1 - 3 are Cs-I Mn-1.78(II) Mn-0.78(III) (0.22)[Fe-II(CN)(6)], Cs-I Mn-1.57(II) Mn-0.57(III) (0.43)[Fe-II(CN)(6)], and Cs-I Mn-1.51(II) Mn-0.51(III) (0.49) [Fe-II(CN)(6)], respectively. The XRD measurements for 1 - 3 show that crystal structures of the HT and LT phases are cubic structures (Fm (3) over barm), but the lattice constants decrease from the HT phase to the LT phase; a = 10.5446( 17) --> 10.4280(7) angstrom ( 1), 10.5589(17) --> 10.3421(24) angstrom (2), and 10.5627(11) --> 10.3268(23) angstrom ( 3). The magnetization vs. temperature curves and the magnetization vs. external magnetic field curves show that the LT phases are ferromagnetic with Curie temperatures of 4.3 ( 1), 5.0 ( 2), and 5.6 K ( 3). At a cooling rate of - 0.5 K min(-1), 4 does not show the charge-transfer phase transition, but does show a behavior of zero thermal expansion with a thermal expansivity of + 0.2 x 10(-6) K-1 throughout the temperature range 300 and 20 K.
机译:制备了一系列的六氰合铁酸铯锰。 (Cs1.78MnII)-Mn-I [Fe-II(CN)(6)](0.28)[Fe-III(CN)(6)](0.22)(1),Cs-I Mn-1.57(II) [Fe-II(CN)(6)](0.57)[Fe-III(CN)(6)](0.43)(2),Cs-1 Mn-1.51(II)[Fe-II(CN)(6) )](0.51)[Fe-III(CN)(6)](0.49)(3)和Cs-1 Mn-0.94(II)[Fe-II(CN)(6)](0.21)[Fe- III(CN)(6)](0.70)中心点0.8H(2)O(4)。图1-3显示了高温(HT)和低温(LT)相之间的电荷转移相变,其转变温度(T-1 / 2向下箭头,T-1 / 2向上箭头)为(207 K, 225 K)(1),(190 K,231 K)(2)和(175 K,233 K)(3)在0.5 K min(-1)的冷却和加热速率下。可变温度红外光谱表明1-3的LT相的化合价态为Cs-I Mn-1.78(II)Mn-0.78(III)(0.22)[Fe-II(CN)(6)],Cs- I Mn-1.57(II)Mn-0.57(III)(0.43)[Fe-II(CN)(6)]和Cs-1 Mn-1.51(II)Mn-0.51(III)(0.49)[Fe- II(CN)(6)]。 1-3的XRD测量表明HT和LT相的晶体结构是立方结构(在巴姆以上的Fm(3)),但是晶格常数从HT相到LT相逐渐减小。 a = 10.5446(17)-> 10.4280(7)埃(1),10.5589(17)-> 10.3421(24)埃(2)和10.5627(11)-> 10.3268(23)埃(3) 。磁化强度与温度的关系曲线以及磁化强度与外部磁场的关系曲线表明,LT相具有居里温度为4.3(1),5.0(2)和5.6 K(3)的铁磁性。在-0.5 K min(-1)的冷却速率下,4不显示电荷转移相变,但确实显示零热膨胀行为,且热膨胀率为+ 0.2 x 10(-6)K-1在300至20 K的整个温度范围内。

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