Nitrogen-induced enhancement of the electron effective mass in InNxAs1−x

2002 ◽  
Vol 80 (5) ◽  
pp. 796-798 ◽  
Author(s):  
W. K. Hung ◽  
K. S. Cho ◽  
M. Y. Chern ◽  
Y. F. Chen ◽  
D. K. Shih ◽  
...  
Keyword(s):  
Effective Mass ◽  
Electron Effective Mass

Nitrogen composition dependence of electron effective mass inGaAs1−xNx

2010 ◽  
Vol 82 (12) ◽  
Author(s):  
T. Dannecker ◽  
Y. Jin ◽  
H. Cheng ◽  
C. F. Gorman ◽  
J. Buckeridge ◽  
...  
Keyword(s):  
Effective Mass ◽  
Composition Dependence ◽  
Electron Effective Mass

Temperature dependence of the electron effective mass in InSb

1974 ◽  
Vol 9 (2) ◽  
pp. 568-571 ◽  
Author(s):  
E. S. Koteles ◽  
W. R. Datars
Keyword(s):  
Temperature Dependence ◽  
Effective Mass ◽  
Electron Effective Mass

The effect of electron effective mass mismatch on electron - phonon scattering rate in a quantum well

1997 ◽  
Vol 12 (3) ◽  
pp. 296-299 ◽  
Author(s):  
Zheng Yisong ◽  
Lu Tianquan ◽  
Wang Yiding ◽  
Wu Xuhong ◽  
Zhang Chengxiang ◽  
...  
Keyword(s):  
Quantum Well ◽  
Effective Mass ◽  
Phonon Scattering ◽  
Electron Effective Mass ◽  
Scattering Rate ◽  
Electron Phonon Scattering

Determination of the Conduction Band Electron Effective Mass in Hexagonal GaN

1995 ◽  
Vol 34 (Part 2, No. 9B) ◽  
pp. L1178-L1179 ◽  
Author(s):  
M. Drechsler ◽  
D. M. Hofmann ◽  
B. K. Meyer ◽  
T. Detchprohm ◽  
H. Amano ◽  
...  
Keyword(s):  
Effective Mass ◽  
Conduction Band ◽  
Electron Effective Mass ◽  
Band Electron ◽  
Conduction Band Electron

NEGATIVE DIFFERENTIAL VELOCITY IN ARTIFICIAL CRYSTALS PROBED BY HIGH MAGNETIC FIELDS

2009 ◽  
Vol 23 (12n13) ◽  
pp. 2766-2768
Author(s):  
A. PATANÈ
Keyword(s):  
Electrical Conductivity ◽  
Electric Field ◽  
Electronic Properties ◽  
Effective Mass ◽  
Conduction Band ◽  
Impurity Level ◽  
Frequency Range ◽  
Electron Effective Mass ◽  
N Level ◽  
Relief Effect

Progress in the synthesis and engineering of semiconductor materials has led to improved device performances and functionalities. In particular, in the last decade, there has been considerable interest in the physics and applications of highly-mismatched alloys in which small and highly-electronegative isovalent N -atoms are incorporated onto the anion sublattice of a III-V compound semiconductor.1 The most studied material is the GaAs 1-x N x alloy. Our magnetotunnelling studies have shown that a small percentage of N (x < 1%) perturbs dramatically the electronic properties of the host GaAs crystal leading to a large increase of the electron effective mass and an unusual response of the energy-wavevector dispersions to hydrostatic pressure.2–6 These effects differ from the smoother variation of the energy band gap and electron effective mass with alloy composition observed in other semiconductor compounds, such as In y Ga 1-y As . The incorporation of N in GaAs gives rise to a qualitatively different type of alloy phenomenon: N -impurities and N -clusters tend to localize the extended Bloch states of GaAs at resonant energies in the conduction band (CB), thus fragmenting the energy-wavevector dispersion relations. The possibility of tailoring the electronic properties of III-V compounds by N -incorporation has stimulated proposals for innovative devices in optoelectronics and high frequency (terahertz, THz) electronics.7 However, to date, the implementation of dilute nitrides in these technologies presents several challenges, including a degradation of the electron mobility. Also, despite a rapidly expanding body of work on the electronic properties of GaAs 1-x N x, the range of N -concentrations over which this alloy behaves as a good conductor is not yet well established. Our magnetotransport experiments have revealed how the incorporation of N in GaAs affects the electrical conductivity. Our studies in n-type GaAs 1-x N x epilayers revealed a large increase of the resistivity, ρ, for x > 0.2%, which we have attributed to the emergence of defect states with deep (~ 0.3 eV) energy levels. Electron trapping onto these states was not observed at low x (x = 0.2%). In this ultra-dilute alloy regime and at low electric fields (F < 1 kV / cm ) the electrical conductivity retains the characteristic features of transport through extended states, albeit with relatively low mobility (µ ~ 0.1 m 2/ Vs at RT) due to scattering of electrons by N -atoms. We have focused our research on this ultra-dilute regime and exploited the admixing of the localized single N -impurity level with the extended conduction band states of GaAs to realize an unusual type of negative differential velocity (NDV) effect: at large F (> 1 kV / cm ), electrons gain sufficient energy to approach the energy of the resonant N -level, where they become spatially localized.7–10 [Formula: see text] This Resonant Electron Localization in Electric Field, to which we give the acronym RELIEF, leads to NDV and strongly non-linear current-voltage characteristics. We envisage that the RELIEF-effect could be observed in other III-N-V alloys, such as InP 1-x N x and InAs 1-x N x. In these compounds the nature of the resonant interaction between the N -level and the conduction band states of the host-crystal is still relatively unexplored. However, it is clear that the different energy positions of the N -level relative to the conduction band minimum of different materials could offer new degrees of freedom in the design of the electronic band structure and electron dynamics. The RELIEF-effect may open up prospects for future applications in fast electronics. We have shown that the maximum response frequency, fmax, of a RELIEF-diode can be tuned by the applied electric field in the THz frequency range.7 This is of potential technological significance for the development of detectors/sources in the 0.6-1 THz region, which is not currently attainable using conventional Transferred Electron Devices and Quantum Cascade Lasers. Our recent studies of GaAs 1-x N x have also shown a fast response of the current in the sub-THz frequency range.11 Experiments involving diodes optimized for THz-operation coupled with a quantitative theoretical model of the THz dynamics will be now needed to assess the use of GaAs 1-x N x and other III-N-V alloys in detectors/sources of THz radiation. Note from Publisher: This article contains the abstract only.

The electron effective mass at the bottom of the GaNAs conduction band

2004 ◽  
Vol 19 (10) ◽  
pp. 1189-1195 ◽  
Author(s):  
C Skierbiszewski ◽  
I Gorczyca ◽  
S P epkowski ◽  
J usakowski ◽  
J Borysiuk ◽  
...  
Keyword(s):  
Effective Mass ◽  
Conduction Band ◽  
Electron Effective Mass
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