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Online since: August 2015
Authors: Rosari Saleh, Shofianina Jalaludin, Sarah A. Arifin
The X-ray diffraction patterns were analyzed by means of the MAUD program using Rietveld whole profile fitting to determine the crystal structure and lattice parameters.
The patterns of pure Fe3O4, TiO2 and CuO nanoparticles were marked and all peaks can be indexed as the typical cubic spinel, anatase structure and monoclinic, respectively.
Comparative mechanistic and kinetic investigations, Journal of Photochemical and Photobiology A: Chemistry. 130 (2000) 35-47
Amighian, A novel non-thermal process of TiO2-shell coating on Fe3O4-core nanoparticles, Journal of Physics and Chemistry of Solids. 73 (2012) 1066–1070
Shen, Influences of different synthesis conditions on properties of Fe3O4 nanoparticles, Materials Chemistry and Physics 113 (2009) 46-52
Online since: September 2005
Authors: N. Vukelić, Zoran Nedić, J. Krstić, A. Milutinović-Nikolić, A. Šućurović, D. Jovanović
Jovanović1 1 Institute of Chemistry Technology and Metallurgy, Department of Catalysis and Chemical Engineering, Njegoševa 12, 11000 Belgrade, Serbia and Montenegro 2 Faculty of Physical Chemistry, University of Belgrade, Serbia and Montenegro a jkrstic@nanosys.ihtm.bg.ac.yu Keywords: Characterization, Nickel Precursor, Sodium Silicate Solution, Synthesis Paths.
A Philips PW 1710 X-ray powder diffraction spectrometer with copper anticathode (λ=0.154178 nm) operating at 40 kV and 30 mA was used to estimate the fraction of amorphous structure.
Second diffuse peak in the 33-45º range with a maximum at 0.256 nm shows the presence of amorphous structure compounds formed in the process of precursor synthesis [9].
Therefore, by adding the precipitation agent drop-by-drop into the first stage of synthesis highly developed porous structure was formed.
Rosic, Proc.6th International Conference on Fundamental and Applied Aspects of Physical Chemistry, Serbia (2002), p. 195
Online since: July 2012
Authors: Xiang Hui Bu, Yan Liu, Qing Jie Sun, Liu Xiong
Amide had three existing forms, which were primary-amide, secondary-amide and tertiary-amide, whose structure forms were RCONH2, R-CO-NHR’ and R-CO-NR’R’, respectively [12].
Journal of Agriculture and Food Chemistry 24 (2): 359-365
Food Chemistry, 127, 1438–1443
Food Chemistry, 70, 139–145
Fourier Transform Infrared Spectroscopic Analysis of Protein Secondary Structures.
Online since: March 2024
Authors: Matanat Mehrabova, Amdulla Mekhrabov
First, compared to CZT, the bond ionicity of CMT is higher, entailing a greater tendency for crystallization into a hexagonal structure, but not in the expected zinc-blende structure.
Magniudes of g-factor, the superhyperfine structure area and the width of individual superhyperfine structure lines for second peak were determined as g= 2.007, A≈ 65.5 G and ~22.1 G, respectievly.
Hasanov, On the growth, structure, and surface morphology of epitaxial CdTe films.
Chauhan, High dose gamma ray exposure effect on the properties of CdSe nanowires, Radiation Physics and Chemistry, 144 (2018) 405-412
Mutharasu, An effect of N+ ion bombardment on the CdTe thin films, Radiation Physics Chemistry, 81.2 (2012) 201-207
Online since: December 2014
Authors: David Marton, Vladimir Modrak
Then, all possible structures for given number of initial nodes can be created.
· to calculate a total structural complexity of an original structure.
Then, to measure sub-structure complexity of original ASC structure, a Module Degree parameter shall be used.
,r) of given Non-modular structure (see Fig. 4b).
Rouvray (Eds.), Complexity in Chemistry, Biology and Ecology, Springer, New York, 2005, pp. 191–235
Online since: January 2009
Authors: Shao Yi Wu, Zhi Hong Zhang, Yue Xia Hu, Xue Feng Wang
In the calculations, the trigonal field parameters  and ' are determined from the superposition model and the local structures of Ni2+ in the halides.
Up to now, however, the above EPR experimental results have not been theoretically interpreted, and the local structure properties around Ni2+ in these materials have not been analyzed, either.
Hong: Chinese Journal of Structural Chemistry.
Wyckoff, Crystal Structures, 2nd ed, (Wiley, New York, 1964) Vol.
Weast: CRC Handbook of Chemistry and Physics (CRC Press, Boca Raton, 1989) p.
Online since: January 2017
Authors: Emmanuel Iwuoha, Anovuyo Jonnas, Candice Rassie, Juanita Van Wyk, Priscilla Baker, Lindsay Wilson, Rachel Fanelwa Ajayi, Nomaphelo Ntshongontshi, Usisipho Feleni
UV-VIS Spectrophotometric Detection Candice Rassie1,a, Juanita Van Wyk2,b, Lindsay Wilson1,c, Nomaphelo Ntshongontshi1,d, Anovuyo Jonnas1,e, Usisipho Feleni1,f, Rachel Fanelwa Ajayi1,g, Priscilla Baker1,h, Emmanuel Iwuoha1,i 1Sensorlab, Department of Chemistry, University of the Western Cape, Bellville, 7535, Cape Town, South Africa 2Department of Chemistry, University of the Witwatersrand, Johannesburg, South Africa.
The HR-SEM images reveal a roughly globular structure of agglomerated particles.
The appearance of lattice fringes as shown in Figure 4(C) confirm the crystalline structure.
Metal centred dendrimers have previously been proven to form crystalline structures [18].
Goddard, “Starburst Dendrimers: Molecular-Level Control of Size, Shape, Surface Chemistry, Topology, and Flexibility from Atoms to Macroscopic Matter,” Angew.
Online since: October 2010
Authors: Susana Orozco, María de los Ángeles Ortiz, Rosa María Méndez-Moreno, Pablo de la Mora, Gabriela Murguía-Romero
These layered structures of high-Tc materials suggest that two-dimensional physics is important in the study of HTSC.
Electronic structure calculations using WIEN2k code [6] for the iron oxypnictide LaO1-xFxFeAs have been done.
The energy band structure for LaO1-xFxFeAs for (left) and (right).
Jónsson, in: Theoretical Methods in Condencsed Phase Chemistry, edited by S.D.
Schwartz, volume 5 of Progress in Theoretical Chemistry and Physics, chapter, 10, Kluwer Academic Publishers (2000)
Online since: August 2014
Authors: Ya Ping Zhu, Kang Kang Guo, Hui Min Qi, Shuai Yong Jin, Fan Wang
The insoluble solid is transformed to Si3N4 and BN amorphous structures with an approximately 95% ceramic yield after being pyrolyzed to 1000˚C.
The chemical structure of PBSZ precursor was also confirmed by 1H NMR spectra, which was shown in Fig. 2.
The resonance at 4.7ppm was attributed to SiH2, and 4.3 ppm was attributed to SiH3 due to rearrangement of polymer structure. 11B and 29Si NMR spectrum were also used to further confirm the structure of PBSZ precursor.
It could be clearly seen that the structure of cured PBSZ after pyrolysis was particularly compact and without any defect.
Besides, the cured PBSZ could maintain the stability of its structure during ceramic reaction and exhibited excellent properties of ceramic conversion.
Online since: September 2011
Authors: Jie Yun Chang, Xiao Bing Zuo, Rong Xin Yuan, Ai Ying Li
For example, with the same overall molecular weight a linear polymer has, hyperbranched polymers possess a significantly lower viscosity, thereby, as a novel pathway to enhance synthetic polymer functions in the fields of coatings, drug delivery systems, supramolecular chemistry, nanotechnology, etc [1-2].
The HBPS-1 molecules with a globular structure, which have a lower contacting surface area, may cause a disruption or change in the surface interaction, creating less overall adhesion.
In other words, such a globular structure may possibly induce the occurrence of slip.
One factor is the HBPS-1 has a globular shape structure with a highly branched and the absence of chain entanglements between the HBPS-1.
Another factor is that HBPS-1 has much lower intrinsic viscosities than PC, due to their relatively lower molecular weights and denser structures when compared with PC.