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Online since: February 2008
Authors: Vladimir V. Popov, E.N. Popova, A.K. Shikov, E.P. Romanov, S.V. Sudareva, E.A. Dergunova, A.E. Vorobyova, S.M. Balaev
., Szulzyk A. et al.: IEEE Trans.
Vol. 27 (1991), p. 2027 [2] Nikulin A., Shikov A., Silaev A et al: IEEE Trans.
et al.: J. of Nuclear Materials Vol. 263 (1998), p. 1929 [4] Popova E.N., Sudareva S.V., Romanov E.P. et al.: Phys.
S15 [7] Wu W., Dietderich D.R., Holthuis J.T. et al.: J.
A, 1994, Vol. 25A, p. 203 [15] Rumaner L.E., Benz M.G. and E.L.
Vol. 27 (1991), p. 2027 [2] Nikulin A., Shikov A., Silaev A et al: IEEE Trans.
et al.: J. of Nuclear Materials Vol. 263 (1998), p. 1929 [4] Popova E.N., Sudareva S.V., Romanov E.P. et al.: Phys.
S15 [7] Wu W., Dietderich D.R., Holthuis J.T. et al.: J.
A, 1994, Vol. 25A, p. 203 [15] Rumaner L.E., Benz M.G. and E.L.
Online since: July 2015
Authors: Florin Miculescu, Ruxandra Vidu, Maria-Diana Vrânceanu, George Tepes, Alecs Matei, Dionezie Bojin, Cosmin Mihai Cotruț
Ghaddar et.al [21] also reported that Ni NWs obtained in their work had larger diameter then the membrane pore.
Eroms et al., “Quantum transport in ferromagnetic permalloy nanostructures,” Physical Review B, vol. 78, no. 17, pp. 174424, 11/24/, 2008
Khatri et al., “Magnetic nanowires by electrodeposition within templates,” physica status solidi (b), vol. 247, no. 10, pp. 2364-2379, 2010
El Jouad, N.
Gieraltowski et al., “Magnetic crossover effect in Nickel nanowire arrays,” Physica B: Condensed Matter, vol. 406, no. 10, pp. 2046-2053, 2011.
Eroms et al., “Quantum transport in ferromagnetic permalloy nanostructures,” Physical Review B, vol. 78, no. 17, pp. 174424, 11/24/, 2008
Khatri et al., “Magnetic nanowires by electrodeposition within templates,” physica status solidi (b), vol. 247, no. 10, pp. 2364-2379, 2010
El Jouad, N.
Gieraltowski et al., “Magnetic crossover effect in Nickel nanowire arrays,” Physica B: Condensed Matter, vol. 406, no. 10, pp. 2046-2053, 2011.
Online since: October 2013
Authors: Xian Gang Wang
Ding et al. proposed that the violet peak (410 nm, 3.03 eV) originated from the electron transition from the bottom of conduction band to the shallow acceptor level formed by Zn vacancies[28]，while Wei et al. proposed that peak at 405nm (3.07 eV) has been attributed to transition from oxygen-vacancy related shallow donor level to valence band[29].
Wei et al. considered that the emission at 486 (2.55 eV) nm may be caused by the electronic transition from the shallow conduction band level to acceptor level of OZn[26], while Ding et al. ascribed the luminescence centered 492 (2.5 eV) nm to the electron transition from the Zn interstitial levels to Zn vacancies[28, 30].
Pal et al. indicated that the emission at about 2.48 eV associated with the recombination of singly ionized oxygen vacancy (VO) electron with pump excited holes in the valence band[31].
Xu et al.[32] had calculated the energy levels of defects in ZnO thin films by using FP-LMTO calculation.
El-Shaer, A.
Wei et al. considered that the emission at 486 (2.55 eV) nm may be caused by the electronic transition from the shallow conduction band level to acceptor level of OZn[26], while Ding et al. ascribed the luminescence centered 492 (2.5 eV) nm to the electron transition from the Zn interstitial levels to Zn vacancies[28, 30].
Pal et al. indicated that the emission at about 2.48 eV associated with the recombination of singly ionized oxygen vacancy (VO) electron with pump excited holes in the valence band[31].
Xu et al.[32] had calculated the energy levels of defects in ZnO thin films by using FP-LMTO calculation.
El-Shaer, A.
Online since: May 2020
Authors: A.K. Kairakbaev, E. S. Abdrakhimova, V.Z. Abdrakhimov
Imangazin, et al., Innovative Directions for Utilization of Ferrous Metallurgy Waste in Ceramic Brick Production, Metallurgist. 61.1-2 (2017) 111-115
Boltakova, et al., Utilization of inorganic industrial wastes in producing construction ceramics.
Azarov, et al.
El-Kheshen, Thermal and chemical properties of diopside-wollastonite glass-ceramics in the SiO2–CaO–MgO system from raw materials, Ceramics international. 29.3 (2003) 265-269
Turki, et al., Multidiscipline Modeling in Materials and Structures, Materials and Structures. 13.2 (2017) 284-296.
Boltakova, et al., Utilization of inorganic industrial wastes in producing construction ceramics.
Azarov, et al.
El-Kheshen, Thermal and chemical properties of diopside-wollastonite glass-ceramics in the SiO2–CaO–MgO system from raw materials, Ceramics international. 29.3 (2003) 265-269
Turki, et al., Multidiscipline Modeling in Materials and Structures, Materials and Structures. 13.2 (2017) 284-296.
Online since: July 2012
Authors: Han Dong Yan, Yu Fei Wang, Zhi Long Quan
Zhao et al. [19] research the effect of raw material ratio and reaction condition for the dispersibility of this superplasticizer.
Zhang et al. [20] call this method as method of fractional steps.
According to above procedure, Zhang et al. [23] synthesized the resin which has a water reducing ratio of approximately 30.5%.
Its performance was researched by Ban et al. [24].
El-Dieb: Cement & Concrete Composites Vol. 32(2010), p. 392 [27] M.S.
Zhang et al. [20] call this method as method of fractional steps.
According to above procedure, Zhang et al. [23] synthesized the resin which has a water reducing ratio of approximately 30.5%.
Its performance was researched by Ban et al. [24].
El-Dieb: Cement & Concrete Composites Vol. 32(2010), p. 392 [27] M.S.
Online since: September 2011
Authors: Zhen Yu Wang, Jia Li, Min Zhe Li, Tong Cun Zhang
Subtilisin inhibitory activity was assayed by the method of Hatakeyama et al [9] and Bubnis and Ofner [10] using succinylcasein and TNBS.
Papain inhibitory activity was determined according to the procedure of Rickauer et al [11] using BAEE as a substrate.
Cathepsin D inhibitory activity was assayed by the method of Yasuda et al [12] using Bz-RGFFP-4-MeObNA as a substrate.
For trypsin and chymotrypsin inhibitory activity staining, gels were treated according to the procedure of Altpeter et al [15].
El-Naggar, and G.
Papain inhibitory activity was determined according to the procedure of Rickauer et al [11] using BAEE as a substrate.
Cathepsin D inhibitory activity was assayed by the method of Yasuda et al [12] using Bz-RGFFP-4-MeObNA as a substrate.
For trypsin and chymotrypsin inhibitory activity staining, gels were treated according to the procedure of Altpeter et al [15].
El-Naggar, and G.
Online since: May 2021
Authors: Sook Keng Chang, Hong Ngee Lim, Zulkarnain Zainal, Laimy Mohd Fudzi, Suhaidi Shafie
According to Kowalik et al. [7], electrodeposition of electrolyte bath was initiated once the electrode was applied with potential that was more negative than the ion’s equilibrium potential characteristic.
Crystallite size calculated from this study was smaller than values reported by Lohar et al. [12] and Yudar et al. [5] as there are many factors that contributed to the differences, which are temperature of heat treatment, deposition rate and so on.
Moreover, the band gap energy of sample electrodeposited at -0.7 V (2.97 eV) has the closest value to that of ZnSe/ZnO to that reported by Chen et al., which is 2.7 eV [14].
These findings are in agreement with Lohar et al. and to Riveros et al. [15] and good quality films of ZnSe can be formed between potential range from -0.7 V to -1.1 V.
El. 28(3) (2017) 2833-2837
Crystallite size calculated from this study was smaller than values reported by Lohar et al. [12] and Yudar et al. [5] as there are many factors that contributed to the differences, which are temperature of heat treatment, deposition rate and so on.
Moreover, the band gap energy of sample electrodeposited at -0.7 V (2.97 eV) has the closest value to that of ZnSe/ZnO to that reported by Chen et al., which is 2.7 eV [14].
These findings are in agreement with Lohar et al. and to Riveros et al. [15] and good quality films of ZnSe can be formed between potential range from -0.7 V to -1.1 V.
El. 28(3) (2017) 2833-2837