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Online since: November 2013
Authors: Divine Ojuh, Nnamdi Omehe
Lachebi et al [18] in their full potential linearised augmented plane wave method obtained 0.16 eV and 4.52 eV for the direct and indirect band gap respectively.
Lachebi et al obtained 4.44 eV for the direct band gap and 8.81 eV for the indirect band gap.
El Haj Hassan, First principles calculations of structural, electronic, optical and thermodynamic properties of PbS, SrS and their ternary alloys Pb1-xSrxS, computational mater.
Lachebi et al obtained 4.44 eV for the direct band gap and 8.81 eV for the indirect band gap.
El Haj Hassan, First principles calculations of structural, electronic, optical and thermodynamic properties of PbS, SrS and their ternary alloys Pb1-xSrxS, computational mater.
Online since: September 2011
Authors: Roland Grössinger, Nasir Mehmood, Rieko Sato Turtelli, Muhammad Aamir Raza, Sohail Afzal Khan, Sajid Raza Choudry
Lograsso, "Magnetoelasticity of Fe-Ga and Fe-Al alloys," J. of Magnetism and Magnetic Materials, vol. 226-230, (2001/5 2001) 948-949
Schlagel, D.L., "Magnetostrictive properties of body-centered cubic Fe-Ga and Fe-Ga-Al alloys," Magnetics, IEEE Transactions on, vol. 36 (2000) 3238-3240
El Hilo, T.
Schlagel, D.L., "Magnetostrictive properties of body-centered cubic Fe-Ga and Fe-Ga-Al alloys," Magnetics, IEEE Transactions on, vol. 36 (2000) 3238-3240
El Hilo, T.
Online since: May 2021
Authors: Marat N. Niyazov, Buvkhan G. Taipova, Anatoliy I. Kupchishin
Research Investigation of Deformation Characteristics of Thin Polymer Films at Different Doses of Electron Irradiation
Niyazov M.N.1,a, Kupchishin A.I.1,2,b, Taipova B.G.1,c
1Kazakh National Pedagogical University named after Abai, Almaty, Kazakhstan
2Kazakh National University named after al-Farabi, Almaty, Kazakhstan
amarat--90@mail.ru, bankupchishin@mail.ru, cbuv_7@mail.ru
Keywords: polytetrafluoroethylene, electron irradiation, mechanical properties, stress, exponential model, radiation dose.
El-Diasty, A.M.
Pilko, Influence of Parameters of Reactive Magnetron Sputtering on Tribomechanical Properties of Protective Nanostructured Ti–Al–N Coatings, Journal of Friction and Wear. 39 2 (2018) 92-98
El-Diasty, A.M.
Pilko, Influence of Parameters of Reactive Magnetron Sputtering on Tribomechanical Properties of Protective Nanostructured Ti–Al–N Coatings, Journal of Friction and Wear. 39 2 (2018) 92-98
Online since: April 2019
Authors: M.R. Sahar, Sulhadi Sulhadi, Syariffah Nurathirah Syed Yaacob, E.S. Sazali
This is possibly attributed to the transformation of (BO) into (NBO) in the doped CuO NPs glass structure as discuss by Nehal et al. [15].
Veeraiah, Specific features of photo and thermoluminescence of Tb3+ ions in BaO – M2O3 ( M = Ga , Al , In )– P2 O 5 glasses, J.Lumin. 127 (2007) 637–644. doi:10.1016/j.jlumin.2007.03.011
El-Aal, H.A.
Veeraiah, Specific features of photo and thermoluminescence of Tb3+ ions in BaO – M2O3 ( M = Ga , Al , In )– P2 O 5 glasses, J.Lumin. 127 (2007) 637–644. doi:10.1016/j.jlumin.2007.03.011
El-Aal, H.A.
Online since: September 2008
Authors: Bruno Tourneret, Pascal Jehanno, Hans Peter Martinz, Brigitte Nigg
LOM of a cross section of siliconized MoSiB - 1
Table.2 Overview of layers formed during siliconizing and oxidation (x no data available)
Siliconizing and Oxidation ( 700 and 900°C) Results
substrate Description of layers after Description of layers after Description of layers after
siliconizing (from cross oxidation at 700°C (from cross oxidation at 900°C (from cross
sections via LOM/SEM/EDX) sections via LOM/SEM/EDX) sections via LOM/SEM/EDX)
W deform W-Si (45 μm) W-Si (40 μm) + W-Si-O (10 - W-Si (37 μm), below: another
25 μm) above W-Si (1μm) with less Si
W sint 92% W-Si (33 μm) with Al-Si-O in- W-Si (35 μm) + W-Si-O (20 - Rests of W-Si (40 - 50 μm),
clusions or topcoat 25 μm) above strong oxidation of W
D 185 W-Si (50 μm) with Ni-Fe-Si- x strong destruction
inclusions and W-Fe-Ni interlayer
(2 - 8 μm)
D 185 chamf W-Si (37 μm) with Ni-Fe-Si- W-Si-Ni-Fe (17 μm) + W-Si-O x
inclusions and W-Fe-Ni inter- (35 -40 μm) above
layer (
2 - 10 μm) D 176 W-Si (35 μm) with Ni-Fe-Si- x strong destruction inclusions and W-Fe-Ni interlayer (15 μm) D 176 chamf W-Si (13 μm) with Ni-Fe-Si- W-Si-Ni-Fe (17 μm) + W-Si-Ni- x inclusions and W-Fe-Ni inter- Fe-O (8 - 20 μm) above layer (10 - 15 μm) D2M W-Si (100 μm) with Ni-Fe-Si- W-Si-Fe-Ni (10 μm) + W-Si-O W-(Mo) (75 μm) + W-Si-O inclusions and W-Fe-Ni-(Mo) (50 -70 μm) + Si-O above (80 -90 μm) + W-Si-Fe-Ni-(Mo) interlayer (15 μm) -O-inclusions W-10Cu Molten Cu-Si (70 - 250 μm) + strong destruction strong destruction transition zone with partially dissolved W-Si-grains (65 μm) Mo Mo-Si (25 μm) Mo-Si (30 μm) Mo-Si (30 μm), below: another Mo-Si (4 μm) with less Si MoSiB Mo-Si (30 μm) Mo-Si (35 μm) + uneven Si-Al- Mo-Si (27 μm), below: another O (15 -40 μm) Mo-Si (2 μm) with less Si Table 2 also includes descriptions of the layers which were formed on the disks during oxidation in air for one week at 700 and 900°C respectively.
Rapp and E.L.
2 - 10 μm) D 176 W-Si (35 μm) with Ni-Fe-Si- x strong destruction inclusions and W-Fe-Ni interlayer (15 μm) D 176 chamf W-Si (13 μm) with Ni-Fe-Si- W-Si-Ni-Fe (17 μm) + W-Si-Ni- x inclusions and W-Fe-Ni inter- Fe-O (8 - 20 μm) above layer (10 - 15 μm) D2M W-Si (100 μm) with Ni-Fe-Si- W-Si-Fe-Ni (10 μm) + W-Si-O W-(Mo) (75 μm) + W-Si-O inclusions and W-Fe-Ni-(Mo) (50 -70 μm) + Si-O above (80 -90 μm) + W-Si-Fe-Ni-(Mo) interlayer (15 μm) -O-inclusions W-10Cu Molten Cu-Si (70 - 250 μm) + strong destruction strong destruction transition zone with partially dissolved W-Si-grains (65 μm) Mo Mo-Si (25 μm) Mo-Si (30 μm) Mo-Si (30 μm), below: another Mo-Si (4 μm) with less Si MoSiB Mo-Si (30 μm) Mo-Si (35 μm) + uneven Si-Al- Mo-Si (27 μm), below: another O (15 -40 μm) Mo-Si (2 μm) with less Si Table 2 also includes descriptions of the layers which were formed on the disks during oxidation in air for one week at 700 and 900°C respectively.
Rapp and E.L.
Online since: March 2016
Authors: Yue Guang Chen, Shi Jiao Wang, Gui Fang Liu
Zhang Wei et al. also studied the microwave absorbing properties of barium ferrite powders.
El-Sayed, T.
Rana, Magnetic and microwave attenuation behavior of Al-substituted Co2W hexaferrites synthesized by sol-gel autocombustion process, Curr.
El-Sayed, T.
Rana, Magnetic and microwave attenuation behavior of Al-substituted Co2W hexaferrites synthesized by sol-gel autocombustion process, Curr.
Online since: May 2014
Authors: Vili Kesti, A. Kaijalainen, A. Väisänen, A.M. Arola, K. Mäntyjärvi, R. Ruoppa, A. Järvenpää, A. Määttä
Chemical composition and mechanical properties of Optim 960QC. [5]
C, max
Si, max
Mn, max
P, max
S, max
Ti, max
CEV, typical
YS, Mpa
TS, Mpa
El, %
CV -40C, J/cm2
0.11
0.25
1.2
0.02
0.01
0.07
0.52
960
1000
7
34
Advantages of the ultra-high-strength level (>900MPa) can be fully utilized only if fabricated properties are on a sufficient level.
Transformation texture components {001}<110>, {113}<110> and {001}<113> in Optim® 960QC (Fig. 3d) are similar as Ray et al. [14] observed in 870°C FRT steel.
According to Yamazaki et al. [17, 18] bendability has no correlation with total elongation, but it is closely related to local elongation.
Transformation texture components {001}<110>, {113}<110> and {001}<113> in Optim® 960QC (Fig. 3d) are similar as Ray et al. [14] observed in 870°C FRT steel.
According to Yamazaki et al. [17, 18] bendability has no correlation with total elongation, but it is closely related to local elongation.