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1.
The high-pressure behaviour of Bi2Fe4O9 was analysed by in situ powder and single-crystal x-ray diffraction and Raman spectroscopy. Pressures up to 34.3(8) GPa were generated using the diamond anvil cell technique. A reversible phase transition is observed at approximately 6.89(6) GPa and the high-pressure structure is stable up to 26.3(1) GPa. At higher pressures the onset of amorphization is observed. The crystal structures were refined from single-crystal data at ambient pressure and pressures of 4.49(2), 6.46(2), 7.26(2) and 9.4(1) GPa. The high-pressure structure is isotypic to the high-pressure structure of Bi2Ga4O9. The lower phase transition pressure of Bi2Fe4O9 with respect to that of Bi2Ga4O9 (16 GPa) confirms the previously proposed strong influence of cation substitution on the high-pressure stability and the misfit of Ga3+ and Fe3+ in tetrahedral coordination at high pressure. A fit of a second-order Birch–Murnaghan equation of state to the p–V data results in K0 = 74(3) GPa for the low-pressure phase and K0 = 79(2) GPa for the high-pressure phase. The mode Grüneisen parameters were obtained from Raman-spectroscopic measurements.  相似文献   

2.
Using density functional theory plus Hubbard U calculations, we show that the ground state of (Mg,Fe)(Si,Fe)O(3) perovskite, the major mineral phase in Earth's lower mantle, has high-spin ferric iron (S=5/2) at both dodecahedral (A) and octahedral (B) sites. With increasing pressure, the B-site iron undergoes a spin-state crossover to the low-spin state (S=1/2) between 40 and 70 GPa, while the A-site iron remains in the high-spin state. This B-site spin-state crossover is accompanied by a noticeable volume reduction and an increase in quadrupole splitting, consistent with recent x-ray diffraction and M?ssbauer spectroscopy measurements. The anomalous volume reduction leads to a significant softening in bulk modulus during the crossover, suggesting a possible source of seismic-velocity anomalies in the lower mantle.  相似文献   

3.
Formation of elongated nanoparticles was observed when was precipitated from solutions containing excess of Fe2+. The average diameter of the particles was 23 nm; the length to diameter ratio was up to 14. This shape was an unexpected phenomenon because bar- or needle-like nanoparticles have been earlier reported only for Fe(III)-based materials. Chemical analysis revealed Fe(OH)2 nature of the obtained particles. In addition, this conclusion was verified with a new simple method for quantitative evaluation of the particle morphology. Application of this method to the mixed samples allowed to distinguish between the two different compounds and to attribute different morphologies to Fe(OH)2 or Results indicate that bars are frequent shapes of nano-sized iron oxides/hydroxides.  相似文献   

4.
利用傅里叶变换近红外光谱分析技术, 对源自国内外不同产地的软玉进行了测试与分析。结果表明在7 000~7 400 cm-1波数范围内,部分产地的软玉中出现四个由羟基倍频振动致近红外吸收谱带,分别归属OH(Mg MgMg),OH(MgMgFe2+),OH(MgFe2+Fe2+),OH(Fe2+Fe2+Fe2+)的倍频振动所致, 并与软玉中透闪石矿物晶体结构中M1和M3位置的Mg2+,Fe2+占位有关。随着透闪石中Fe2+/(Fe2++ Mg2+)比值的增大,亦可导致软玉中羟基NIR谱带的进一步分裂,谱带数目和强度增加,并向低波数方向位移。文中对软玉中羟基NIR光谱的产地鉴别意义一并给予了讨论。  相似文献   

5.
利用发射光谱研究脉冲电晕放电中的自由基   总被引:10,自引:2,他引:10  
利用发射光谱技术在大气压下测量了以氮气为载气的不饱和水蒸气体系针-板式正脉冲电晕放电产生的OH(A^2∑→X^2Ⅱ0—O)自由基和O(3p^5P→3s^5S^02777.4nm),Ha(3P→2S 656.3nm)活性原子的发射光谱,并由N2(C^3Ⅱu→B^3Ⅱg)的△v=-3和△v=-4振动带序发射光谱强度计算得出N2(C,v)的相对振动布居及其振动温度,进而采用高斯分布拟合准确地求出了N2(C^3Ⅱu→B^3Ⅱg)的△v= 1振动带序发射光谱强度,从而可以由N2(C^3Ⅱu→B^3Ⅱg)的△v= 1振动带序与OH(A^2∑→X^2Ⅱ0—0)的重叠发射光谱中准确求出OH(A^2∑→X^2Ⅱ0—0)自由基的发射光谱强度。由发射光谱强度得到了激发态OH(A^3∑)自由基和O(3p^5P),Ha(3P)活性原子的布居。还研究了激发态OH(A^2∑)自由基和O(3p^5P),Ha(3P)活性原子的布居随放电电压和放电频率的变化以及氧气对激发态OH(A^2∑)自由基和O(3p^5P),Ha(3P)活性原子布居的影响。  相似文献   

6.
合成了4种新的糖胺 金属配合物,分别为[Ni(HL) (H2 O) 2 ]2 Cl2 ·CH3OH·2H2 O ,[Cu(HL) ]2 Cl2 ·CH3CH2 OH·3H2 O ,[Zn(HL) ]2 Cl2 ·H2 O ,[Co(HL) (H2 O) (OH) ]2 Cl2 ·CH3OH·2H2 O (HLN ,N′ 二βD 葡萄糖基乙二胺) ,并用元素分析、红外、紫外、核磁共振氢谱对其结构进行了表征。结果表明,Ni(Ⅱ) ,Co(Ⅲ)配合物为八面体构型,而Cu(Ⅱ) ,Zn(Ⅱ)配合物为四面体构型。最后研究了其对对硝基苯吡啶甲酸酯(PNPP)催化水解的催化速率常数。  相似文献   

7.
Abstract

A phase transition from Ca(OH)2 I (portlandite) to Ca(OH)2 II at high pressure and temperature has been confirmed, using in situ x-ray diffraction in a multianvil high pressure device (DIA). The structure was determined at 9.5 GPa and room temperature from data collected after heating the sample at 300°C at 7.2 GPa in a diamond anvil cell. Both the Le Bail fit and preliminary Rietveld refinement suggest that the new phase, which reverts to Ca(OH), I during pressure release, has a structure related to that of baddeleyite (ZrO1); it is monoclinic (P21/c) with a= 4.887(2), b= 5.834(2), c = 5.587(2), β = 99.74(2)°. The coordination number of Ca increases from six to seven (5 + 2) across the transition. At 500°C, the phase boundary is bracketed at 5.7 ± 0.4 GPa by reversal experiments performed in the DIA.  相似文献   

8.
The high-temperature behavior of bafertisite was studied by combination of techniques in order to characterize the temperature-induced iron oxidation associated with deprotonation of an octahedral layer. The chemical formula of bafertisite from Darai-Pioz alkaline complex (Tajikistan) determined by electron-microprobe analyzes and Mössbauer spectroscopy is Ba 2.11(Fe\({}_{2.70}^{2+}\)Fe\({}_{0.17}^{3+}\)Mn 1.09Zr 0.04Na 0.03) (Ti 1.96Nb 0.07)(Si 2 O 7)2 O 2(OH 1.29 O 0.65 F 0.06)F 2. In situ high-temperature powder X-ray diffraction revealed abrupt shift of reflections to the high-angle region and reduction of their intensity at T >?525 °C. The Mössbauer spectroscopy studies indicated that the crystal structure of bafertisite contains Fe in octahedral sites as predominantly ferric ions with Fe 3+/ ΣFe =?0.06, whereas bafertisite annealed at T =?600 °C has Fe in the same position with Fe 3+/ ΣFe up to 0.39. The differential scanning calorimetry and thermogravimetric analyzes reveal the occurrence of a broad exothermic effect at T ~ 537 °C associated with the mass loss corresponding to deprotonation. Since in the studied sample of bafertisite, Fe 2+ apfu strongly prevails over OH apfu, the stoichiometric (charged-balanced) high-temperature oxidized modification cannot be obtained. In the paper, the high-temperature behavior of bafertisite is discussed and compared to that of astrophyllite.  相似文献   

9.
“黑碧”指颜色为黑色,主要成分为阳起石的碧玉。电子探针、激光剥蚀电感耦合等离子体质谱仪分析显示“黑碧”为阳起石碧玉。拉曼光谱和红外光谱的OH振动处产生3个主峰,归属于MgMgMg-OH,MgMgFe2+-OH(Fe2+M1MgM1MgM3-OH,MgM1MgM1Fe2+M3-OH),MgFe2+Fe2+-OH(MgM1Fe2+ M1Fe2+M3-OH,Fe2+M1Fe2+M1MgM3-OH),但与常见和田玉不同,“黑碧”的三个主峰在拉曼光谱OH的振动区(3 600~3 700 cm-1)和红外光谱OH的倍频振动区(7 200~7 100 cm-1)产生分裂现象。将“黑碧”分为5个区域:HB-1,HB-2,HB-3,HB-4和HB-5,进行原位的电子探针和拉曼光谱分析,拉曼光谱在3 600~3 700 cm-1出现3个主峰(A,B,C),将主峰进行分峰拟合处理,显示分裂成6个次级峰(A′和A″,B′和B″,C′和C″),次级峰之间的平均波数差为5 cm-1。前人对角闪石在OH振动处主峰分裂现象的观点各不相同。结合“黑碧”的原位电子探针数据和相关研究文献,认为角闪石中B(M4)位置上的阳离子分布是分裂谱产生的主要原因。角闪石中的B(M4)位置虽然没有直接与W位置的OH相连接,但B(M4)位置上的阳离子通过影响TO4上的桥氧,间接影响W位置上的OH,从而引起OH振动光谱产生一定变化。对比存在类似分裂谱的角闪石样品和“黑碧”的晶体化学式,发现所有的样品在B(M4)位置上均存在Ca2+和Mn2+分布,而其他位置的阳离子占位情况都不相同,表明“黑碧”OH振动光谱产生分裂与B(M4)位置上的Ca2+和Mn2+分布有关。故认为“黑碧”中OH振动光谱产生分裂原因为Ca2+和Mn2+在B(M4)位置上的占位,且高波数峰位归属于Ca2+,低波数峰位归属于Mn2+,即A′,B,C′归属于Ca2+,A″,B″,C″归属于Mn2+。  相似文献   

10.
Mössbauer spectra of green rust one run at 78 and 4.4 K exhibit two ferrous and one ferric sites in the 2/1/1 intensity ratio. Chemical formula is set at 3Fe(OH)2, Fe(OH)2Cl, nH2O. By replacing Fe2+ with Ni2+ ions, the compound is stabilized and the structure is determined on a ABiBCiCai stacking sequence. Space group is P3121 with an hexagonal unit cell of parameters a=6.17 and c=23.5 A0.  相似文献   

11.
选取产自广西大化瑶族自治县岩滩镇的黑青色阳起石玉为研究对象,采用电子探针、傅里叶变换红外光谱仪和激光拉曼光谱仪就其化学成分和振动光谱特征进行测试分析,并对小半径金属阳离子在阳起石晶体结构中的占位情况予以讨论。结果表明,广西黑青色阳起石玉的主要矿物组成为富铁阳起石,并含有少量铁阳起石;化学成分中的高含量FeOT(Wt%:18.596%~26.791%)是导致其折射率值(1.64)、密度值(3.12 g·cm-3)偏高且在自然光下呈黑色、透射光下呈绿色的主要原因。受晶体结构中Fe2+对Mg2+的类质同象替代作用影响,广西黑青色阳起石玉1 400~400 cm-1范围内的红外吸收谱带与100~1 200 cm-1范围内的拉曼谱峰位置较透闪石向低频区发生偏移,频差不等;且中红外、近红外吸收光谱和拉曼光谱中均可见四个(MgMgMg)OH(A带),(MgMgFe2+)OH(B带),(MgFe2+Fe2+)OH(C带)和(Fe2+Fe2+Fe2+)OH(D带)振动谱带,其中基频振动谱带分别位于3 674,3 660,3 644和3 625 cm-1附近,倍频振动谱带分别位于7 183,7 154,7 118和7 077 cm-1附近,相对强度为A<D<B<C。化学成分和M-OH红外振动谱带积分面积计算结果显示广西黑青色阳起石玉晶体结构中Mg2+优先占据M2位置,Fe2+优先占据M1位置;Mg2+和Fe2+在M1和M3位置上的分布相对有序,占位系数接近于1。综合分析认为广西黑青色阳起石玉的变质程度属绿片岩相范畴。  相似文献   

12.
The electron spin states of iron in minerals of the Earth’s mantle at high pressures mostly determine the physicochemical properties of deep layers of the Earth and are of great interest not only for geophysics but also for fundamental physics of strongly correlated electron systems. In this work, using Raman and synchrotron Mössbauer nuclear forward scattering (NFS) spectroscopies, iron-containing magnesium–silicate perovskite (Mg, Fe)SiO3 (10% Fe) has been studied in the cryogenic temperature range of 35–300 K and at high pressures up to 48 GPa, which are created in diamond anvil cells. The analysis of NFS spectra has indicated that iron ions are in a nonmagnetic (para- or diamagnetic) state in the entire region of temperatures and pressures and the electronic properties can be controlled by means of the quadrupole splitting parameter. It has been found that an increase in the pressure and a decrease in the temperature are accompanied by a significant increase in the parameter Δ from 2 mm/s to ~4 mm/s, which indicates that the electronic state of Fe2+ ions changes. The maximum Δ value has been observed at P > 20 GPa, but the pressure behavior of a transition strongly depends on the temperature. Possible mechanisms of the transition have been discussed.  相似文献   

13.
The crystallographic structure of Ni(II)?Fe(III) hydroxy-chloride green rusts obtained by oxidation of a FexNi1?x(OH)2 precipitate is isomorphous with that of the ferrousferric green rust one and independent of the value of P=Fe/Ni. Mössbauer spectra exhibit two quadrupole doublets after further oxidation of the compounds which correspond to a formula (3-x)Ni(OH)2 · xFeOOH · Fe(OH)2Cl. The Fe3+ ions are found to occupy preferentially the sites close to the Cl? ions and the Ni2+ those far from them. However the ordering of the Fe3+ ions is not perfect.  相似文献   

14.
张钊  崔航  杨大鹏  张剑  汤顺熙  吴思  崔啟良 《中国物理 B》2017,26(10):106402-106402
The structural compression mechanism and compressibility of gallium oxyhydroxide, α-GaOOH, are investigated by in situ synchrotron radiation x-ray diffraction at pressures up to 31.0 GPa by using the diamond anvil cell technique. Theα-GaOOH sustains its orthorhombic structure when the pressure is lower than 23.8 GPa. The compression is anisotropic under hydrostatic conditions, with the a-axis being most compressible. The compression proceeds mainly by shrinkage of the void channels formed by the coordination GaO_3(OH)_3 octahedra of the crystal structure. Anomaly is found in the compression behavior to occur at 14.6GPa, which is concomitant with the equatorial distortion of the GaO_3(OH)_3 octahedra. A kink occurs at 14.6 GPa in the plot of finite strain f versus normalized stress F, indicating the change in the bulk compression behavior. The fittings of a second order Birch–Murnaghan equation of state to the P–V data in different pressure ranges result in the bulk moduli B_0= 199(1) GPa for P 14.6 GPa and B_0= 167(2) GPa for P 14.6 GPa. As the pressure is increased to about 25.8 GPa, a first-order phase transformation takes place, which is evidenced by the abrupt decrease in the unit cell volume and b and c lattice parameters.  相似文献   

15.
杭锦2#土是内蒙古鄂尔多斯杭锦旗地区发现的层状含铁天然矿物,利用X射线衍射、吡啶吸附红外光谱及X射线光电子能谱技术对样品的性质进行了表征。X射线光电子能谱表明杭锦2#土骨架结构中Si和Al原子结合能与标准硅氧四面体和铝氧八面体中Si和Al结合能相比明显增加,表面存在Lewis酸位和Brönsted酸位,且杭锦2#土中铁物种以Fe(Ⅲ)和Fe(Ⅱ)形式存在于骨架结构中;非均相Fenton反应中杭锦2#土的Fe(Ⅱ)可与H2O2反应生成自由基(·OH)与Fe(Ⅲ),但反应速率慢且难以循环。酸活化后杭锦2#土中Si和Al的结合能进一步增加,铁物种部分转变为非结构铁并以Fe3+与Fe2+转移到样品表面;X射线光电子能谱、吡啶红外和氨气程序升温表征表明酸活化杭锦2#土表面Lewis酸位和Brönsted酸位增多;非均相Fenton反应中,酸活化杭锦2#土表面Fe3+与Fe2+可与H2O2循环反应,不断生成·OH并对甲基橙进行降解,且活化杭锦2#土表面Brönsted酸能够提供质子将H2O2包围,抑制其分解生成HO-2并提供更多的·OH,Lewis酸能增加杭锦2#土表面吸附氧(Oad)含量,而Fe2+可被Oad氧化为Fe3+,促进Fe2+/Fe3+之间的循环,同时在氧化过程中电子转移到Oad形成O·-2,O·-2能够与Brönsted酸提供的质子反应形成·OH,·OH与O·-2均为氧化性自由基,能够提升活化杭锦2#土非均相Fenton反应活性。此外,X射线衍射表明酸活化使杭锦2#土中CO2-3转化为对Fenton反应负面影响更小的SO2-4进而提升其非均相Fenton反应活性。  相似文献   

16.
Molecular Diversity - Agar-coated Fe3O4 nanoparticles (Fe3O4@agar) were prepared simply through in situ co-precipitation of Fe2+ and Fe3+ ions via NH4OH in an aqueous solution of Agar. Coating of...  相似文献   

17.
Cation distributions and related order-disorder phenomena in the naturally occurring Mn-spinels: iwakiite, galaxite and franklinite, have been investigated by means of57Fe Mössbauer spectroscopy. Previous measurements on an iwakiite sample indicated the existence of Mn-rich and Mn-poor regions. This interpretation has been confirmed in this investigation by further measurements on annealed iwakiite samples. The57Fe Mössbauer spectrum of galaxite from Bald Knob, NC, is a well-resolved quadrupole doublet and indicates the presence of a single crystallographic Fe3+ species. A galaxite sample from Thailand exhibited a complex spectrum of Fe2+ and Fe3+ quadrupole doublets: This sample has been misidentified and should be regarded as a member of the (Mg, Fe)(Al, Fe)2O4 series. The57Fe hyperfine parameters of a rare franklinite from Längban, Sweden, are very close to those for synthetic zinc ferrite, confirming electron microprobe results of an unusually high zinc content.  相似文献   

18.
A high-pressure 57Fe Mössbauer study of SrFeO3 up to 74 GPa has been performed with diamond-anvil-cell (DAC) using synchrotron radiation and a radioactive point source of 57Co in Rh. SrFeO3 is known as a typical cubic perovskite with a high-valence state of Fe4+ and shows metallic conductivity at 0.1 MPa down to 4.2 K. Applying an external high pressure, SrFeO3 has not shown any structural transformation up to 74 GPa keeping an Fe4+ state but the Néel temperature increases up to 300 K at 18 GPa. The external high pressure may induce the ferromagnetism in SrFeO3 by a decrease of the interatomic distance of Fe or an increase of the d-band width. 57Fe Mössbauer measurements under externally applied longitudinal magnetic field using radioactive 57Co in Rh source and also nuclear forward scattering measurements with a linearly polarized synchrotron radiation under external magnetic field indicate the existence of the pressure induced ferromagnetism in SrFeO3. In this work we compare high-pressure Mössbauer spectroscopy using synchrotron and radioactive sources and summarize the advantages and disadvantages of each method.  相似文献   

19.
Fe40Ni40P12B8非晶合金的冲击晶化实验研究   总被引:9,自引:2,他引:7       下载免费PDF全文
 本文研究了Fe40Ni40P12B8非晶合金冲击波加载下的晶化行为,冲击波由二级轻气炮发射的告诉弹丸撞击靶产生。实验结果表明:Fe40Ni40P12B8非晶合金在冲击波加载下,晶化可在加载时间(微秒量级)内发生;晶化的阈值压力在30~50 GPa之间,相应的冲击温度约为510~800 K,晶化析出相与冲击压力有关,低压下析出相是面心立方γ-(Fe, Ni)固溶体和Fe3(P0.37B0.63)化合物,高压下(大于60 GPa)析出相除了面心立方γ-(Fe, Ni)固溶体和Fe3(P0.37B0.63)化合物之外,还包括(Fe, Ni)3P化合物。  相似文献   

20.
Herein, a simple in situ charge/discharge activation strategy is proposed to synthesize Fe(OH)3 film on Fe foam as an efficient anode of supercapacitors. The physical characteristics of electrodes are characterized and the electrochemical energy storage performances are investigated. Importantly, it is demonstrated the as‐synthesized Fe(OH)3@Fe foam electrode adopted a novel Fe3+/Fe0 redox reaction mechanism for energy storage in alkaline electrolytes. Compared with previously reported Fe3+/Fe2+ mechanisms, the Fe3+/Fe0 redox couple shows a more promising application value (e.g., higher theoretical‐specific capacitance, excellent conductivity of its reduction state). As for supercapacitor anodes, the electrode achieves high areal capacitance of 5.55–3.94 F cm−2 at a current range of 20–200 mA cm−2 and shows good stability for high‐rate and long‐term cycling. The assembled single supercapacitor device gives a high energy density of 11.64–7.43 Wh m−2 at a power density of 157–1461 W m−2. More importantly, the as‐adopted in situ activation strategy may also have potential value for synthesizing other transition metal oxide‐based products.  相似文献   

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