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1.
    
The transition of disc‐like chromium hydroxide nanomaterials to chromium oxide nanomaterials has been studied by hot‐stage Raman spectroscopy. The structure and morphology of α‐CrO(OH) synthesised using hydrothermal treatment were confirmed by X‐ray diffraction (XRD) and transmission electron microscopy (TEM). The Raman spectrum of α‐CrO(OH) is characterised by two intense bands at 823 and 630 cm−1 attributed to ν1 CrIII O symmetric stretching mode and the band at 1179 cm−1 attributed to CrIII OH δ deformation modes. No bands are observed above 3000 cm−1. The absence of characteristic OH stretching vibrations may be due to short hydrogen bonds in the α‐CrO(OH) structure. Upon thermal treatment of α‐CrO(OH), new Raman bands are observed at 599, 542, 513, 396, 344 and 304 cm−1, which are attributed to Cr2O3. This hot‐stage Raman study shows that the transition of α‐CrO(OH) to Cr2O3 occurs before 350 °C. Copyright © 2010 John Wiley & Sons, Ltd.  相似文献   

2.
    
Titanium substituted chromium oxide (Cr2 − xTixO3 + z, CTO) has gained increasing interest concerning gas sensing applications. CTO is prepared by synthesis of chromium oxide and titanium oxide. Different techniques for verification of successful synthesis of CTO have been investigated. Solid state Fourier transform infrared spectroscopy (FTIR) and Raman spectroscopy were performed in addition to the common analysis via X‐ray diffraction (XRD). The spectroscopic methods offer a fast, qualitative verification of a complete synthesis. CTO was synthesized in a high temperature sintering step, and powders and dispersions of CTO were prepared. A high energy grinding process leads to the required particle size reduction. The size distribution and crystallite size of the CTO particles were measured. Furthermore morphology and surface coverage analysis on novel type gas‐sensing CTO layers, deposited via inkjet technology, were performed and specific adsorption energies of nitrogen dioxide on printed CTO layers were derived. High porosity with sub‐micron particles was shown to be characteristic for the layers, resulting in a highly sensitive gas‐sensing behavior, with 500 ppb of nitrogen dioxide being clearly detectable.  相似文献   

3.
    
Cr2O3 nanoparticles, widely used in the industry, can be obtained by calcination of the nanoparticles synthesized via the hydrothermal method. The chemical nature and the morphology of as‐prepared and calcined nanoparticles are investigated by scanning electron microscopy, X‐ray diffraction and Raman spectroscopy. Our results indicate that the as‐prepared nanoparticles mainly consist of amorphous and hydrated Cr(OH)3, with only minor amounts of Cr2O3. By contrast, and as already known before, calcined nanoparticles consist of Cr2O3. We also demonstrate the effect of inappropriately chosen experimental conditions, because the use of laser intensities above 0.7 mW during the Raman experiments causes a local heating and thus induces the transformation of Cr(OH)3 into Cr2O3. The correlation between the laser power and a local heating is further corroborated by thermogravimetric analyses, which show that upon increased temperature, Cr(OH)3 first dehydrates and then partially condensates to the intermediate CrO(OH) form, to finally attain the crystalline form of Cr2O3 at about 409 °C. Copyright © 2017 John Wiley & Sons, Ltd.  相似文献   

4.
    
Pure nesquehonite (MgCO3·3H2O)/Mg(HCO3)(OH)·2H2O was synthesised and characterised by a combination of thermo‐Raman spectroscopy and thermogravimetry with evolved gas analysis. Thermo‐Raman spectroscopy shows an intense band at 1098 cm−1, which shifts to 1105 cm−1 at 450 °C, assigned to the ν1CO32− symmetric stretching mode. Two bands at 1419 and 1509 cm−1 assigned to the ν3 antisymmetric stretching mode shift to 1434 and 1504 cm−1 at 175 °C. Two new peaks at 1385 and 1405 cm−1 observed at temperatures higher than 175 °C are assigned to the antisymmetric stretching modes of the (HCO3) units. Throughout all the thermo‐Raman spectra, a band at 3550 cm−1 is attributed to the stretching vibration of OH units. Raman bands at 3124, 3295 and 3423 cm−1 are assigned to water stretching vibrations. The intensity of these bands is lost by 175 °C. The Raman spectra were in harmony with the thermal analysis data. This research has defined the thermal stability of one of the hydrous carbonates, namely nesquehonite. Thermo‐Raman spectroscopy enables the thermal stability of the mineral nesquehonite to be defined, and, further, the changes in the formula of nesquehonite with temperature change can be defined. Indeed, Raman spectroscopy enables the formula of nesquehonite to be better defined as Mg(OH)(HCO3)·2H2O. Copyright © 2008 John Wiley & Sons, Ltd.  相似文献   

5.
    
Changes of different chromium oxide species [Cr(VI), Cr(V) and Cr(III)] were investigated using in situ Raman spectroscopy in an anhydrous hydrogen fluoride (AHF) atmosphere. It was found that the Cr(VI) (CrO3) and Cr(V) (YCrO4) species were easy to fluorinate, and generated CrO2F2 or/and CrOF3, while the Cr(III) (Cr2O3) species was difficult to fluorinate. Moreover, the CrO2F2 and CrOF3 species were stable in the AHF atmosphere, but they easily transform into CrO3 in N2 atmosphere and further decomposed to Cr2O3 at 400 °C. Moreover, Cl/F exchange reaction of CF3CH2Cl to CF3CH2F over these Cr species indicated that the high‐oxidation‐state CrOxFy (CrO2F2 and CrOF3) species exhibited much higher reactivities than Cr2O3, suggesting that these species (CrO2F2 and CrOF3) may be the active phases of the reaction. Copyright © 2010 John Wiley & Sons, Ltd.  相似文献   

6.
Designing a structure having high local field enhancement, wideband resonance, and large hot spot area is the key element to obtain a large enhancement factor for surface-enhanced Raman spectroscopy applications. Here, the concentric toroid structures in dimer configuration is proposed, which shows a large local field intensity in a wide spectral range and the region that leads to a high-surface-enhanced Raman scattering signal intensity. Calculations show that the average surface-enhanced Raman scattering enhancement is up to 60 times more compared to the conventional dimer toroid structures with similar size.  相似文献   

7.
测量了七种非理想化学计量比的UO2+x(0<x<0.66)及UO2和U3O7等理想化学计量比氧化铀的拉曼和红外光谱,并进行了对比分析,其中U3O7和U3O8之间UO2+x的分子振动光谱为首次报道。拉曼光谱结果显示,随着UO2+xx值的增加,UO2特征峰中的578和1 150 cm-1峰强度快速减弱,当x=0.19时,这两峰基本消失,可视为准完美萤石晶体结构UO2的标志。445 cm-1峰强度在减弱的同时变宽并偏移,当x=0.32时,该峰已偏移至459 cm-1处,同时在~630 cm-1出现一弱肩峰,这与四方相U3O7的特征峰一致。当x≥0.39时,459 cm-1峰发生分裂,在235和754 cm-1处出现新峰并增强,其特征逐渐与正交相的α-U3O8接近。但直至x=0.60时,与α-U3O8相比其333,397,483和805 cm-1峰仍不突出。红外光谱结果显示,随着UO2+xx值的增加,UO2位于400~570 cm-1区间的强吸收特征谱带逐渐分裂为~421和~515 cm-1两峰并增强,同时UO2在~700 cm-1的弱吸收峰逐渐消失,~645 cm-1处的肩峰逐渐显现,出现的这三个峰正是U3O7的特征红外吸收峰。当x≥0.39时,在744 cm-1出现一强吸收峰并增强,该峰是α-U3O8的最强特征峰。但即使x=0.60时,~645 cm-1峰仍然存在,同时~515 cm-1峰也未明显分裂成485和535 cm-1峰,这表明UO2.60仍处于四方相和正交相的过渡阶段。上述结果表明,随着x值的增加,UO2+x的晶体结构发生变化,每次变化均在拉曼和红外光谱中得到体现。通过对比各特征峰相对强度和位置的变化情况,可很好区分和表征不同的氧化铀。  相似文献   

8.
    
Frank J. Owens 《Molecular physics》2013,111(11):1280-1283
It has been proposed that reduction of exfoliated graphite oxide could be a potential method for producing large quantities of graphene. Raman and surface-enhanced Raman spectroscopy are used to show that oxidation of graphite and exfoliated graphite significantly increases the defect structure of both materials. This would likely lead to a heavily defected graphene structure when oxygen is removed. To insure the observed decomposition is not due to the laser light, the effect of laser intensity on the materials was investigated. It was found that at the highest laser intensity (1.4 × 108 W/M2) there was a significant increase in defects. However, lower laser intensity was found which did not produce defects and was used in the studies of the effect of oxidation on the spectra.  相似文献   

9.
The Raman scattering spectra of isostructural Bi2O3 and Bi1.8Tm0.2O3 in the course of heating have been investigated. It is shown that the sequences of structural changes with increase in temperature differ: and * , respectively. In the hightemperature region, the structure takes the form of a disordered cube irrespective of the previous history of specimens.  相似文献   

10.
    
Pb(Fe2/3W1/3)O3 (PFW) thin films were deposited on platinized silicon substrate by a chemical solution deposition technique. Room‐temperature X‐ray diffraction (XRD) revealed a pure cubic crystal structure of the investigated material. The microstructure indicated good homogeneity and density of the thin films. A Raman spectroscopic study was carried out on PFW to study the polar nano‐regions in the temperature range 85–300 K. The Raman spectra showed a change in the peak intensity and a shift towards the lower wavenumber side with temperature. The Raman spectra also revealed the transition from the relaxor to the paraelectric state of PFW. There was no evidence of a soft mode in the low‐temperature region, in contrast to the normal ferroelectric behavior. The polar nano‐regions tend to grow and join at low temperatures (∼85 K), which become smaller with increase in temperature. The presence of strong Raman spectra in the cubic phase of the material is due to the presence of distributed Fm3m(Z = 2) symmetry nano‐ordered regions in the Pm3m(Z = 1) cubic phase. Copyright © 2007 John Wiley & Sons, Ltd.  相似文献   

11.
12.
    
A new Raman spectroscopic setup for in situ characterization of catalytic materials based on a tunable laser system and a confocal Raman microscope is described. The laser excitation wavelength is variable over a broad range from deep ultraviolet (UV) to near‐infrared allowing for targeted use of Raman diagnostics for catalyst characterization. By utilization of resonance effects, the sensitivity of the method can be strongly increased. The potential of the setup is illustrated by new in situ Raman results on dispersed vanadium oxide catalysts obtained at 217.5 and 280 nm UV laser excitation. Copyright © 2013 John Wiley & Sons, Ltd.  相似文献   

13.
Aluminium-doped zinc oxide (ZnO:Al) films were prepared by magnetron sputtering at different radio-frequency powers (Prf) of 50, 100, 150 and 200 W. The properties of the films were characterised by X-ray photoelectron spectroscopy (XPS), atomic force microscopy (AFM), Raman microscopy, and spectrophotometry with the emphasis on the evolution of compositional, surface-morphological, optical, electrical and microstructural properties. XPS spectra showed that within the detection limit the films are chemically identical to near-stoichiometric ZnO. AFM revealed that root-mean-square roughness of the films has almost linear increase with increasing Prf. Optical band gap Egopt of the films increases from 3.31 to 3.51 eV when Prf increases from 50 to 200 W. A widening Egopt of the ZnO:Al films compared to the band gap (∼3.29 eV) of undoped ZnO films is attributed to a net result of the competition between the Burstein-Moss effect and many-body effects. An electron concentration in the films was calculated in the range of 3.73 × 1019 to 2.12 × 1020 cm−3. Raman spectroscopy analysis indicated that well-identified peaks appear at around 439 cm−1 for all samples, corresponding to the band characteristics of the wurtzite phase. Raman peaks in the range 573-579 cm−1 are also observed, corresponding to the A1 (LO) mode of ZnO.  相似文献   

14.
    
We report the synthesis of high‐quality graphene on Cu foils using hot‐filament chemical vapor deposition technique and demonstrate that by suitably varying the CH4 and H2 flow rates, one can also obtain hydrogenated graphene. Micro‐Raman spectroscopy studies confirm the growth of monolayer graphene as inferred from the intensity ratio of 2D to G peak which is nearly four in unhydrogenated samples. Detailed Raman area mapping confirms the uniform coverage of monolayer graphene. The grown layer is also transferred onto a Si substrate over ~10 × 10 mm sq. area. The present results provide a leap in synthesis technology of high‐quality graphene and pave way for scaling up the process. Copyright © 2012 John Wiley & Sons, Ltd.  相似文献   

15.
    
The problem of calculating the long-time-limit effective diffusivity in stable two-phase polycrystalline material is addressed for the first time. We make use of a phenomenological model where the high-diffusivity interphase boundaries are treated as connected ‘coatings’ of the individual grains. The derivation of expressions for the effective diffusivity with segregation is along the lines of the analysis by Maxwell in . Monte Carlo computer simulation using lattice-based random walks on a very fine-grained mesh is employed to test the validity of the expressions. It is shown that, for the specific cases analysed, the derived expressions for the effective diffusivity are in very good agreement with results from the simulations. Since the pattern of behaviour is not entirely clear at present, it is difficult to guide the choice for the best expression in a given case. The equivalent of the Hart equation for this problem is also derived. This equation is shown to be invariably in poor agreement with simulation results.  相似文献   

16.
    
We have investigated ten standard single crystal substrates of complex oxides on the account of their applicability in the Raman spectroscopy‐based thin film research. In this study, we suggest a spectra normalization procedure that utilizes a comparison of the substrate's Raman spectra to those of well‐established Raman reference materials. We demonstrate that MgO, LaGaO3, (LaAlO3)0.3(Sr2AlTaO6)0.7 (LSAT), DyScO3, YAlO3, and LaAlO3 can be of potential use for Raman‐based thin film research. At the same time TiO2 (rutile), NdGaO3, SrLaAlO4, and SrTiO3 single crystals exhibit multiple phonon modes accompanied by strong Raman background that substantially hinder Raman‐based thin film experiments. Copyright © 2014 John Wiley & Sons, Ltd.  相似文献   

17.
    
Thermometry utilizing the vibrational spectrum of nitrogen is a very common tool in combustion diagnostics via spontaneous and coherent Raman scattering spectroscopy. In the presence of strong temperature gradients, however, it is likely that hot and cold gas portions contribute to the signal. This is known as spatial averaging, and it can result in severe measurement errors. The present work proposes and demonstrates two straightforward approaches that allow the identification of spatial averaging as well as estimating the resulting error. For this purpose, simulated Raman spectra are considered in order to avoid any impact from experimental artifacts. The first approach utilizes difference spectra, whereas the second one is based upon principal component analysis (PCA). Two scenarios were tested: (1) spectra of 50:50 mixtures exhibiting a common mean temperature and (2) spectra of mixtures with systematically varied fractions of hot (2000 K) and cold (300 K) gas. It is shown that the resulting measurement error can be as high as 500 K.  相似文献   

18.
A bronze Pan (water vessel), dating back to the 4th–3rd century BC, was excavated at Jiuliandun in Hubei Province, central southern China, in 2002. The Pan attracts wide attention among the Chinese archaeologists and conservators for its uniqueness in style and color, which turns out to be due to a black‐brown film of about 1 mm thickness. In the present work, a combined use of X‐ray fluorescence (XRF), micro‐Raman, and X‐ray diffraction (XRD) was employed to determine both chemical and physical compositions of the Pan's film. The results are summarized as follows: (1) The film, as XRF analysis indicates, has high concentrations of chromium (Cr) and iron (Fe); (2) Both Raman and XRD analyses suggest that the element Cr probably exists in the film mainly in the form of chromium oxide (Cr2O3). Raman analysis also implies the presence of PbCrO4·PbO in the film; (3) XRD analysis suggests that the element Fe exists in the film in the form of magnetite (Fe3O4). Based on these analytical results and Chinese historical records, we propose that, as early as in the 3rd century BC, people in central southern China might have discovered and intentionally used chromium minerals for bronze surface treatment (such as coating). The source of chromium minerals used in this period was likely Cr‐spinel minerals from meteorites. More work remains to be done to test the possibility of using Cr‐spinel minerals for bronze production and decoration. Other issues, such as the possibility of forming a chromium‐rich film during the underground burial, also need to be solved. Copyright © 2011 John Wiley & Sons, Ltd.  相似文献   

19.
Ternary molybdate NaCaGd1−x(MoO4)3:Er3+/Yb3+ phosphors with the proper doping concentrations of Er3+ and Yb3+ (x = Er3+ + Yb3+, Er3+ = 0, 0.05, 0.1, 0.2 and Yb3+ = 0, 0.2, 0.45) were successfully synthesized by microwave sol–gel method for the first time. Well-crystallized particles formed after heat-treatment at 900 °C for 16 h showed a fine and homogeneous morphology with particle sizes of 3–5 μm. The optical properties were examined comparatively using photoluminescence emission and Raman spectroscopy. Under excitation at 980 nm, the doped particles exhibited a strong 525-nm emission band, a weak 550-nm emission band in the green region, which correspond to the 2H11/2  4I15/2 and 4S3/2  4I15/2 transitions, and a very weak 655-nm emission band in the red region, which corresponds to the 4F9/2  4I15/2 transition. The optimal Yb3+:Er3+ ratio was obtained to be 9:1, as indicated by the composition-dependent quenching effect of Er3+ ions. The pump power dependence of upconversion emission intensity and Commission Internationale de L’Eclairage chromaticity coordinates of the phosphors were evaluated in detail.  相似文献   

20.
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