2020
DOI: 10.1016/j.physe.2019.113731
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Electronic properties and carrier transport properties of low-dimensional aluminium doped silicene nanostructure

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Cited by 13 publications
(11 citation statements)
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“…Subsequently, the transverse effective masses (in the zigzag direction) of these materials are obtained by using parabolic band approximation. The detailed procedures to obtain the effective masses can be found in Ref [ 33 ]. Although previous work [ 33 ] shows only the modelling procedures for the p-type AlSi 3 nanosheet, the same technique is repeated to compute the electronic properties of n-type PSi 3 nanosheet, in order to obtain both type of transistors for CMOS applications.…”
Section: Modelling Proceduresmentioning
confidence: 99%
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“…Subsequently, the transverse effective masses (in the zigzag direction) of these materials are obtained by using parabolic band approximation. The detailed procedures to obtain the effective masses can be found in Ref [ 33 ]. Although previous work [ 33 ] shows only the modelling procedures for the p-type AlSi 3 nanosheet, the same technique is repeated to compute the electronic properties of n-type PSi 3 nanosheet, in order to obtain both type of transistors for CMOS applications.…”
Section: Modelling Proceduresmentioning
confidence: 99%
“…The detailed procedures to obtain the effective masses can be found in Ref [ 33 ]. Although previous work [ 33 ] shows only the modelling procedures for the p-type AlSi 3 nanosheet, the same technique is repeated to compute the electronic properties of n-type PSi 3 nanosheet, in order to obtain both type of transistors for CMOS applications. Table 1 summarises the important electronic properties of the AlSi 3 and PSi 3 nanosheets, where m 0 is the constant for electron rest mass.…”
Section: Modelling Proceduresmentioning
confidence: 99%
See 1 more Smart Citation
“…The band structures of the defective ZSiNRs are plotted by using the dispersion relation from the solutions of energy eigenvalues from the Hamiltonian matrices. The defective ZSiNRs are modelled using the NNTB approach based on the time-independent Schrödinger in matrix form [15][16][17]: (1) where ℎ( ) is the Hamiltonian matrix, 0 is the time-independent wave function and is the energy. In this work, the Hamiltonian matrix is divided into the -matrix and -matrix which describes the interactions of silicon atoms in the zigzag unit cell chain and the interations among the zigzag unit cell chains respectively.…”
Section: Band Structuresmentioning
confidence: 99%
“…The absence of bandgap in pristine silicene did not halt its exploration for nanotransistor applications. In spite of the challenges, various bandgap engineering techniques have been explored, and such examples include confinement through silicene nanoribbons (SiNRs) [ 18 20 ], co-decoration [ 21 ], and doping [ 22 – 24 ]. Among the aforementioned techniques, doping is the most commonly employed technique in the semiconductor industry to alter the electronic properties [ 25 ].…”
Section: Introductionmentioning
confidence: 99%