2002
DOI: 10.1016/s0038-1101(01)00332-x
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An accurate charge control model for spontaneous and piezoelectric polarization dependent two-dimensional electron gas sheet charge density of lattice-mismatched AlGaN/GaN HEMTs

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Cited by 146 publications
(68 citation statements)
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“…where D ¼ 4pm*/h 2 is the conduction band density of states of a 2-D system, k B is the Boltzmann's constant, m* is the electron effective mass (m* ¼ 0.22m o ), m o is the electron rest mass, h is Planck's constant, T is the absolute temperature, E F is the Fermi energy and the allowed energy levels in the triangular quantum well are E i ¼ c i n s 2/3 (eV) for i ¼ 0.1 with c 0 ¼ 2.123 Â 10 À12 and c 1 ¼ 3.734 Â 10 À12 [10]. Equation (1) shows the relationship between the sheet carrier density, n s , and the Fermi level E f , and assumes a triangular potential well with only the first two quantum states (E 1 and E 0 ) being occupied.…”
Section: A Charge Controlmentioning
confidence: 99%
See 1 more Smart Citation
“…where D ¼ 4pm*/h 2 is the conduction band density of states of a 2-D system, k B is the Boltzmann's constant, m* is the electron effective mass (m* ¼ 0.22m o ), m o is the electron rest mass, h is Planck's constant, T is the absolute temperature, E F is the Fermi energy and the allowed energy levels in the triangular quantum well are E i ¼ c i n s 2/3 (eV) for i ¼ 0.1 with c 0 ¼ 2.123 Â 10 À12 and c 1 ¼ 3.734 Â 10 À12 [10]. Equation (1) shows the relationship between the sheet carrier density, n s , and the Fermi level E f , and assumes a triangular potential well with only the first two quantum states (E 1 and E 0 ) being occupied.…”
Section: A Charge Controlmentioning
confidence: 99%
“…where m is the aluminum mole fraction, e(m) is the dielectric constant of AlGaN, d d is the thickness of the doped AlGaN barrier layer, d i is the thickness of the undoped AlGaN spacer layer, Dd is the effective width of the 2DEG, q is the electron charge, V gs is the applied gate-to-source voltage, and V th (m) is the polarization-dependent threshold voltage given as [10],…”
Section: A Charge Controlmentioning
confidence: 99%
“…(11) we get E 0 (eV ) = 1.35865 × 10 −6 (E well ) 2/3 (12) E 1 (eV ) = 2.39015 × 10 −6 (E well ) 2/3 (13)…”
Section: Dependence Of Eigenenergy On E Wellmentioning
confidence: 94%
“…But charges due to both spontaneous and piezoelectric polarization process are highly responsible for formation of more 2DEG density in AlGaN/GaN system by a factor of 10 over the AlGaAs/GaAs system [11] without the cost of doping. Rashmi et al [12] developed an appropriate charge control model for n s formed in triangular quantum well subject to both strong and weak inversion mode considering polarization charges. But as MOSHEMT state of the art technology is recently developed, till date to the best of the author's knowledge no model explains the dependence of n s on oxide layer parameters.…”
Section: Introductionmentioning
confidence: 99%
“…In 2002, Rashmi [30] deduced some approximate expression from equation (6) appropriating for different region of operation which obviously, is not convenient for application. Although the approximation has improved a lot, but all of above analytical expressions for EF versus ns have been proposed so far have disadvantages more or less, such as can not appropriate for a large range of values of ns, the results are not accurate enough for modeling and so on.…”
Section: Relation Between Fermi Level and Surface Charge Densitymentioning
confidence: 99%