2018
DOI: 10.3938/jkps.72.622
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Wigner Transport Simulation of Resonant Tunneling Diodes with Auxiliary Quantum Wells

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Cited by 6 publications
(4 citation statements)
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“…After resonance voltage, the S-InGaAs valley current density comprises a longer voltage range with a minimum at V = 5.3 V, whereas the Ref-GaAs minimum valley current density is at V = 3.8 V. Moreover, the valley current density is higher for the S-InGaAs sample leading to a lower PVCR at 4 K. At reverse bias voltage, the S-InGaAs peak current density is j res = −8.9 µA/µm 2 at V res = −5.10 V, while the Ref-GaAs peak current density is j res = −51.6 µA/µm 2 at V res = −5.78 V. The heterostructure asymmetry leads to the reduction in the absolute value of the peak current density compared to forward bias, and this reduction is more pronounced for the prewell-containing heterostructure (see Ref. [31]).…”
Section: Resultsmentioning
confidence: 99%
“…After resonance voltage, the S-InGaAs valley current density comprises a longer voltage range with a minimum at V = 5.3 V, whereas the Ref-GaAs minimum valley current density is at V = 3.8 V. Moreover, the valley current density is higher for the S-InGaAs sample leading to a lower PVCR at 4 K. At reverse bias voltage, the S-InGaAs peak current density is j res = −8.9 µA/µm 2 at V res = −5.10 V, while the Ref-GaAs peak current density is j res = −51.6 µA/µm 2 at V res = −5.78 V. The heterostructure asymmetry leads to the reduction in the absolute value of the peak current density compared to forward bias, and this reduction is more pronounced for the prewell-containing heterostructure (see Ref. [31]).…”
Section: Resultsmentioning
confidence: 99%
“…The approaches presented in [12,16] are based on the expansion of the statistical density matrix in terms of the eigenvectors of the diffusion matrix for the case of a simplified Hamiltonian assuming a spatially constant effective mass distribution, which seems to be the standard model for numerical investigations of the Wigner equation, e.g. [14,[17][18][19][20][21][22]. In [23,24], the approach has been analyzed with regard to plane wave functions spanning the numerical basis, which become particular important when multiband transport has to be considered or the spatially varying effective mass has to be taken into account.…”
Section: Introductionmentioning
confidence: 99%
“…Significant progress has been achieved in the electronic structure engineering of nanoscopic systems, allowing for a thorough characterization of the charge carrier dynamics and correlation with the optical response. This is particularly crucial in semiconductor heterostructures like resonant tunneling diodes (RTDs) where challenging questions still pervade the physics of carrier excitation, transport, relaxation, and recombination. In particular, mapping the thermalization gradient along the transport path and how it is affected by external factors is still a relevant topic to be characterized and understood, and optical tools are well suited for this purpose. , …”
Section: Introductionmentioning
confidence: 99%
“…This is particularly crucial in semiconductor heterostruc-tures like resonant tunneling diodes (RTDs) [1][2][3][4][5] where challenging questions still pervade the physics of carrier excitation, transport, relaxation, and recombination. [6][7][8][9][10] In particular, mapping the thermalization gradient along the transport path and how it is affected by external factors is still a relevant topic to be characterized and understood, and optical tools are well suited for that purpose.…”
mentioning
confidence: 99%