Bulk GaN and AlGaN∕GaN heterostructure drift velocity measurements and comparison to theoretical models

2005 ◽  
Vol 97 (6) ◽  
pp. 063705 ◽  
Author(s):  
J. M. Barker ◽  
D. K. Ferry ◽  
D. D. Koleske ◽  
R. J. Shul
1990 ◽  
Vol 43 (6) ◽  
pp. 755 ◽  

The drift velocity of electrons in water vapour at 294 K has been measured over the E/N range 1�4 to 40 Td with an error estimated to be 35 Td. The present data show that J.lN decreases monotonically with decreasing E/N at low E/N values as observed by Wilson et al. (1975) and does not become independent of E/N as indicated by Lowke and Rees (1963). The present values, although lower than those of Lowke and Rees, lie within the combined error limits, except for values below 2 Td. The present data suggest that the momentum transfer cross section at low energies is approximately 10% larger than that obtained by Pack et al. (1962) from their drift velocity measurements.


1983 ◽  
Vol 10 (8) ◽  
pp. 757-760 ◽  
Author(s):  
A. D. M. Walker ◽  
H. Junginger ◽  
O. H. Bauer

2006 ◽  
Vol 24 (9) ◽  
pp. 2375-2389 ◽  
Author(s):  
R. A. Makarevich ◽  
F. Honary ◽  
V. S. C. Howells ◽  
A. V. Koustov ◽  
S. E. Milan ◽  
...  

Abstract. E-region irregularity velocity measurements at large flow angles with the STARE Finland coherent VHF radar are considered in context of the ion and electron velocity data provided by the EISCAT tristatic radar system, CUTLASS Finland coherent HF radar, and IMAGE fluxgate magnetometers. The data have been collected during a special experiment on 27 March 2004 during which EISCAT was scanning between several E- and one F-region altitudes along the magnetic field line. Within the E-region, the EISCAT measurements at two altitudes of 110 and 115 km are considered while the electron velocity is inferred from the EISCAT ion velocity measurements at 278 km. The line-of-sight (l-o-s) VHF velocity measured by STARE VHF los is compared to the ion and electron velocity components (Vi0 comp and Ve0 comp) along the STARE l-o-s direction. The comparison with Ve0 comp for the entire event shows that the measurements exhibit large scatter and small positive correlation. The correlation with Ve0 comp was substantial in the first half of the interval under study when Ve0 comp was larger in magnitude. The comparison with Vi0 comp at 110 and 115 km shows a considerable positive correlation, with VHF velocity being typically larger (smaller) in magnitude than Vi0 comp at 110 km (115 km) so that VVHF los appears to be bounded by the ion velocity components at two altitudes. It is also demonstrated that the difference between VVHF los and Vi0 comp at 110 km can be treated, in the first approximation, as a linear function of the effective backscatter height heff also counted from 110 km; heff varies in the range 108–114 km due to the altitude integration effects in the scattering cross-section. Our results are consistent with the notion that VHF velocity at large flow angles is directly related to the ion drift velocity component at an altitude heff.


1973 ◽  
Vol 26 (6) ◽  
pp. 771 ◽  
Author(s):  
RW Crompton ◽  
MT Elford

The drift velocity of electrons in oxygen at 293 K has been measured over the range 0.8 ≤ E/N ≤ 12 Td by the Bradbury–Nielsen time-of-flight method. The factors governing the range over which measurements can be made are discussed and it is shown that long drift tubes should be used for drift velocity measurements in oxygen at low values of E/N. A 50 cm drift tube is described. The error in the present results is estimated to be less than 1 % for 1.8 E/N E/N > 6 Td and at 1.5 Td, 5 % at 1 Td, and 10 % at 0.8 Td. The present data are in good agreement with those of Fleming et al. (1972) and Nelson and Davis (1972) over the E/N range where the sets of data overlap.


1991 ◽  
Vol 77 (10) ◽  
pp. 763-765 ◽  
Author(s):  
Y. Yang ◽  
J.Y. Lee ◽  
P. Miller ◽  
L. Li ◽  
J. Kumar ◽  
...  

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