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An Al-doped P+ enrichment layer was implanted at high temperature (T) (>500°C) and dose (100% Ref~3x1015 cm-2) inside the P wells in the active area to create a low resistivity ohmic tunnel contact.
High temperature annealing processes increase the activation of Al dopant in the P+ wells, by reducing in this way the P+ contact resistance.
The increase of the Al P+ dose in the enrichment implant inside the P wells is potentially another suitable option to improve surge ruggedness in 4H-SiC MPS diodes.
El-Shawarby, The Influence of Doping Concentration, Temperature, and Electric Field on Mobility of Silicon Carbide Materials, Proc. of 2006 IEEE International Conference on Semiconductor Electronics, Kuala Lumpur, Malaysia, November 2006
Roccaforte, Ohmic Contacts on p-Type Al-Implanted 4H-SiC Layers after Different Post-Implantation Annealings, Materials, 12, (2019), 3468

Elfanaoui1f, Ahmed Ihlal1g 1Materials and Renewable Energy Laboratory, Faculty of Sciences, Ibn Zohr University, Agadir, Morocco 2Université Grenoble Alpes, CNRS, CEA/LETI-Minatec, Grenoble INP, LTM, Grenoble F-38054, France 3MANAPSE Lab, Faculty of Science, Mohammed V University in Rabat, Morocco ahass00.najih@gmail.com, bnabilllebchir@gmail.com, ca.tihane@uiz.ac.ma, da.narjis@uiz.ac.ma, el.atourki@um5r.ac.ma, fa.elfanaoui@uiz.ac.ma, ga.ihlal@uiz.ac.ma Keywords: CH3NH3PbI3 perovskite, Nanorods, Photoluminescence; Raman shift, UV-visible spectrum Abstract.
Chen et al. showed almost the same Raman peaks [28].
Basumaty et al. et Kong et al. found Eg=1.58 eV for the tetragonal structure of MAPI3 films.
Outzourhit, Structural, optical and electrical properties of planar mixed perovskite halides/Al-doped Zinc oxide solar cells.

Wu, Back pressure equal channel angular consolidation of pure Al particles, Scripta Materialia 53(11) (2005) 1225-1229
Xia, Nanostructured Al–Al2O3 composite formed in situ during consolidation of ultrafine Al particles by back pressure equal channel angular pressing, Acta Materialia 57(14) (2009) 4321-4330
Horita, Powder consolidation of Al–10wt% Fe alloy by High-Pressure Torsion, Materials Science and Engineering: A 558 (2012) 462-471
Abd El Aal, E.

Joarder et al. [1]have tried to evaluate the radiation losses but they have also found radiation losses to be negligible .Since radiation is highly spectral, so in order to do the radiation calculations correctly it is necessary to calculate the radiative properties of gases at each and every wavelength point for a large range.
Equilibrium condition data at 0.02 μs has been taken from Joarder et al. [1] to carry out further simulations for the radiation losses( see Table 1) Table 1: Values of various variables at Initial and equilibrium conditions Variable Initial Conditions (entire domain) Equilibrium Conditions (at plasma region) T 300 K 17800 K P 101325 Pa 5071070 Pa N2 0.755 0.325064 O2 0.2322 0.000989 AR 0.0128 0.0128 N 0 0.423377 O 0 0.223719 NO 0 0.014053 Chemical Kinetics As laser energy is deposited, breakdown occurs at the threshold energy and temperature of the focal region starts rising and reaches to a very high value of almost 17800K .At such a high temperature, dissociation of air into various species starts occurring.
The NIST database contains information for line positions (λ), Einstein coefficients, energy of upper and lower transition states(EU , EL ), and the degeneracy of the energy states(gU, gL ).
The radiation loss over the whole simulation time up to 60μs from 0.02μs can be roughly estimated as = 197.35mJ/s x 30μs =5.92 μJ This is the maximum approximate loss .The earlier value for the radiative losses by Jordar et al. was 0.33μJ[1].
Sohn, I., et al., Advanced radiation calculations of hypersonic reentry flows using efficient databasing schemes.

DPPH radical-scavenging activity The DPPH (2, 2-diphenyl-1-picrylhydrazyl) radical scavenging activity of the extracts was measured according to the method of Brand-Williams et al. (1995) [10].
ABTS radical cation-scavenging assay For the ABTS assay, the procedure followed a modified version of Giao et al.’s [11] method.
The data from the present study reveals that the antioxidant activity of different parts of Thai gac fruits is correlated with Kobula et al.
Hung, et al.
El-Missiry, F.M.

Takahashi, et al.: Int.
Zhang, et al.: Key Eng.
Diaz-Arnold, et al.: J.
El-Mowafy, et al.: J.

Elbestawi et al [4] discovered that the different process parameters contributes to the effects on the tool performances, surface finish and integrity of AISI H13 tool steel with having the hardness values of 45 and 55 HRC.
Moreover, Urbanski et al [5] showed investigation on how the milling forces, surface roughness, and tool wear vary with the cutting speed, types of insert, and coating in the milling of hardened AISI H13 tool steel.
D’ Errico et al showed that the coated carbide tool has provide an enhancement to the chip flow results in release of the cutting edges and providing bond of thermally insulated barrier that reject heat from the tool surface into the chips in consequence protecting the tool substrate and making it last longer [9].
A Ghani et al [10] stated that with the high hardness, lower friction coefficient and reduced surface roughness of coated carbide tools has allow the chip to flow off the surface of the tool and therefore reduces the built up edge and wear which thus increases tool life.
Jawahir, I.S.2001, “ Tool wear mechanisms in hard turning with PCBN tools”, Wear 205, pp. 576-586 [4] Elbestawi MA, Chen L, Beeze CE, El-Wardany TI, (1997), High speed of die and mold in their hardened state, A model for chip formation during machining of hardened steel, Annal of CIRP 46:57-62 [5] Urbanski JP, Koshy P, Dewes RC, Aspinwall DK, (2000), High speed machining of moulds and dies for net sharp manufacture.

Gather et al. [9] investigated the important process parameters of hydroforming process for robust parameter design by using the Taguchi method.
Li et al. [12] applied an orthogonal experimental array for FEM simulations of tube hydroforming process.
The fluid pressure and blank holder curves were obtained from a previous study (Halkacı et al. 2011) as shown in Fig.1.
Fluid pressures and blank holder force paths used in the analysis and the experiments (Halkacı et al. 2011) Sixteen simulations were conducted according to L16 orthogonal array as given in Table 2.
El-Sebaie: International Journal of Machine Tools & Manufacture, Vol. 49 (2009), p. 773–780 [4] M.

Monoclinic (m) and tetragonal (t) content were obtained using Toraya et al. [23].
Rejab et al. [29] have also further explained that the increase in fracture toughness can be attributed to the presence of CeO2 in ZTA as this would represent a good solid solubility between Ce4+ and Y3+ in the (Zr,Y,Ce)O2 phase that tends to stabilize the transformation of tetragonal (t) to monoclinic (m) inside ZTA.
Rejab et al further explained that hardness is greatly influeneced by density and increase in hardness was caused by higher densificaions.
Niihara,, Effect of grain morphology and grain size on the mechanical properties of Al 2 O 3 ceramics. 
El-Hout,M.E.S.

Al-Kalali1,a, Mohammed Y.
This trend was also concluded by Meohrjardi et al. [6] who noticed that the layer of geocell was pulled down below the plate (footing) settlement; however, at a remote distance from the loading plate periphery, no tension in the geocell was observed.
As a result, the shear strength is clearly increased and the failure pattern is adjusted as stated in Michalowski and Shi [11] and Fattah et al. [12].
The present results are also compatible with the results of El Sawwaf and Nazir[13] who studied the cyclic settlement behavior of strip footings resting on reinforced layered sand slope, and found that the improving in reducing settlement when the width of geogrid increases is significant until B=2, beyond which the effect on the footing behavior is limited.
Al-Kalali, Three-dimensional finite element simulation of the buried pipe problem in geogrid reinforced soil, Journal of Engineering, University of Baghdad, 22(5) 2016 60-73