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a FT-IR, b Raman, and c UV-Vis absorption spectra with d plots of (αhν)² as a function of energy E for both α-MoO3 nanobelts and h-MoO3 microrods

a FT-IR, b Raman, and c UV-Vis absorption spectra with d plots of (αhν)² as a function of energy E for both α-MoO3 nanobelts and h-MoO3 microrods

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Two modifications of molybdenum trioxide with orthorhombic (α-MoO3) and hexagonal (h-MoO3) crystal structure have been synthesized by a microwave-assisted hydrothermal method, facilitated by formic acid. Characterization by means of X-ray diffraction, scanning electron microscopy, specific surface analysis, and Fourier-transform infrared, Raman, an...

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... Very few reports are available on the synthesis of single crystal strip-like structure of orthorhombic MoO 3 sample [1,16]. There are various methods are available for the synthesis of single crystal a-MoO 3 like ultrasonicassisted [17] hydrothermal [18] spray pyrolysis [19] chemical co-precipitation [20], microwave technique [21], combustion route [22] etc. From these reported methods microwave and co-precipitation method combinly used for the synthesis of a-MoO 3 micro-strips hence called as microwave-assisted chemical co-precipitation method. Microwaves synthesis is rapid method due to its high power densities, fast efficient production which reduces production cost. ...
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The orthorhombic MoO3 micro-strips sample was synthesized using microwave assisted chemical co-precipitation technique. Synchrotron X-ray Diffraction (SXRD) pattern and Rietveld Refinement was used to estimate structural parameter, crystallite size of sample. It reveals that the synthesized sample MoO3 crystallized as an orthorhombic phase. X-ray Absorption Spectroscopy (XAS) measurement, which comprises both X-ray Absorption Near Edge Structure (XANES) and Extended X-ray Absorption Fine Structure (EXAFS) techniques, have been carried out on Mo K-edge to probe the local structure of samples. Local structure is also confirmed from the SXRD and Raman spectra of sample. XAS measurement reveals that the first bond length of Mo-O and Mo-Mo is 1.69 and 3.42 Å in orthorhombic MoO3 respectively. Transmission electron microscopy and SAED patterns showed stripe-like structure and single-crystal formation of MoO3 respectively.
... This may be due to the dielectric relaxation phenomena occurring in the compound [41]. The tangent loss (tanδ) caused by the dipole relaxation phenomena decreases with frequency, as seen in the tanδ frequency plots [42]. which it goes to a lower value. ...
... This may be due to the dielectric relaxation phenomena occurring in the compound [41]. The tangent loss (tanδ) caused by the dipole relaxation phenomena decreases with frequency, as seen in the tanδ frequency plots [42]. ...
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... The sharp absorption edge at 420 nm indicates the visible light absorption. The absorption at this region arises due to the electronic transition from the higher valance band (HOMO level) containing of O 2p orbital hybridized with Mo 4d to the lower conduction band which is composed of Mo 4d (LUMO level) orbital hybridized with O 2p [22]. Kubelka-Munk (K-M) function was employed to estimate the band gap energies of the NPs [23], ...
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... 28,29 The narrow band located at 992 cm −1 is related to asymmetric stretching of the oxygen atoms (MoO) in the α-MoO 3 phase. 30 The intense band appearing at 817 cm −1 is assigned to the Mo-O-Mo symmetric stretching vibrations (or the doubly connected bridge-oxygen Mo-O-Mo), while asymmetric stretching of the triply connected bridge-oxygen Mo 3 -O along the c-axis can be found at 663 cm −1 . 31 Both XRD and Raman results showed the success in obtaining single phase orthorhombic α-MoO 3 structures. ...
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