Abstract:We show that N-polar GaN/(Al, Ga)N/GaN heterostructures exhibit significant N deficiency at the bottom (Al, Ga)N/GaN interface, and that these N vacancies are responsible for the trapping of holes observed in unoptimized N-polar GaN/(Al, Ga)N/GaN high electron mobility transistors. We arrive at this conclusion by performing positron annihilation experiments on GaN/(Al, Ga)N/GaN heterostructures of both N and Ga polarity, as well as state-of-the-art theoretical calculations of the positron states and positronel… Show more
“…In the fast positron setup, a high-purity Ge (HPGe) detector with energy resolution of 1.15 keV at 511 keV was used to record the annihilation photons emitted from two sample pieces with a positron source sandwiched in between. The positron source with 1 MBq of activity was composed of 22 Na encapsulated in 1.5-μm-thick Al-foil. The amount of source annihilations was determined with positron lifetime measurements to be less than 4%.…”
Section: A Sample Orientation In Experimentsmentioning
confidence: 99%
“…Positron annihilation spectroscopy is a nondestructive method with selective sensitivity to neutral and negative vacancy-type defects, and second-order sensitivity to negatively charged defects without open volume [11]. Thanks to these properties, positron annihilation methods have been successful in identifying the role of native point defects in the electrical compensation of n-type doped compound semiconductors such as GaN, ZnO, AlN, InN, and In 2 O 3 [12][13][14][15][16], as well as their alloys such as InGaN and AlGaN [17][18][19][20][21][22]. In spite of the otherwise significant research interest in β-Ga 2 O 3 , the number of reported studies with positron annihilation is surprisingly low [23][24][25][26].…”
We report a systematic first-principles study on positron annihilation parameters in the β-Ga 2 O 3 lattice and Ga monovacancy defects complemented with orientation-dependent experiments of the Doppler broadening of the positron-electron annihilation. We find that both the β-Ga 2 O 3 lattice and the considered defects exhibit unusually strong anisotropy in their Doppler broadening signals. This anisotropy is associated with low symmetry of the β-Ga 2 O 3 crystal structure that leads to unusual kind of one-dimensional confinement of positrons even in the delocalized state in the lattice. In particular, the split Ga vacancies recently observed by scanning transmission electron microscopy produce unusually anisotropic positron annihilation signals. We show that in experiments, the positron annihilation signals in β-Ga 2 O 3 samples seem to be often dominated by split Ga vacancies.
“…In the fast positron setup, a high-purity Ge (HPGe) detector with energy resolution of 1.15 keV at 511 keV was used to record the annihilation photons emitted from two sample pieces with a positron source sandwiched in between. The positron source with 1 MBq of activity was composed of 22 Na encapsulated in 1.5-μm-thick Al-foil. The amount of source annihilations was determined with positron lifetime measurements to be less than 4%.…”
Section: A Sample Orientation In Experimentsmentioning
confidence: 99%
“…Positron annihilation spectroscopy is a nondestructive method with selective sensitivity to neutral and negative vacancy-type defects, and second-order sensitivity to negatively charged defects without open volume [11]. Thanks to these properties, positron annihilation methods have been successful in identifying the role of native point defects in the electrical compensation of n-type doped compound semiconductors such as GaN, ZnO, AlN, InN, and In 2 O 3 [12][13][14][15][16], as well as their alloys such as InGaN and AlGaN [17][18][19][20][21][22]. In spite of the otherwise significant research interest in β-Ga 2 O 3 , the number of reported studies with positron annihilation is surprisingly low [23][24][25][26].…”
We report a systematic first-principles study on positron annihilation parameters in the β-Ga 2 O 3 lattice and Ga monovacancy defects complemented with orientation-dependent experiments of the Doppler broadening of the positron-electron annihilation. We find that both the β-Ga 2 O 3 lattice and the considered defects exhibit unusually strong anisotropy in their Doppler broadening signals. This anisotropy is associated with low symmetry of the β-Ga 2 O 3 crystal structure that leads to unusual kind of one-dimensional confinement of positrons even in the delocalized state in the lattice. In particular, the split Ga vacancies recently observed by scanning transmission electron microscopy produce unusually anisotropic positron annihilation signals. We show that in experiments, the positron annihilation signals in β-Ga 2 O 3 samples seem to be often dominated by split Ga vacancies.
“…[ 61 ] This phenomenon has been very recently utilized to study the atomic‐scale structure of the hole‐attractive interface in N‐polar high electron mobility transistor (HEMT) devices. [ 63 ] Interestingly, the strong 2D confinement caused by the built‐in electric fields enhances the positron sensitivity also to N vacancies that are otherwise essentially invisible to positron annihilation methods, as shown in Figure . This finding opens up new opportunities for using positron annihilation spectroscopy for studying defects and carrier localization phenomena in devices and device‐like heterostructures.…”
Section: Iii‐nitride Alloys and Heterostructuresmentioning
confidence: 99%
“…The experimental "MQW" data are from a specifically designed multiquantum-well structure where positrons annihilate at the interface(s) of interest, showing good agreement with calculated curves for 2-4 V N . Reproduced with permission [63]. Copyright 2020, American Physical Society.…”
Three topical materials systems are discussed from the point of view of point defect characterization with positron annihilation spectroscopy. The family of III‐nitride semiconductors and device structures made thereof poses interesting challenges for data interpretation due to preferential localization and annihilation with various elements. Semiconducting oxides with relatively complex crystal lattice structures further highlight the need for combining systematically designed experiments with state‐of‐the‐art theoretical calculations. High‐entropy alloys generate another challenge due to the large number of randomly distributed elements, combining chemical disorder with structural order.
“…This trend is similar to what has been observed previously in Si-doped AlGaN with 60% Al, 22 while generally from the point of view of electrical compensation, Si doping has not been found to induce high concentrations of cation vacancies in GaN or AlGaN up to 65% Al content. 20,[22][23][24][25][26] It is known that in GaN, 8,27 and particularly in AlN, 10 negative non-open volume defects (negative ions) can effectively trap positrons also at room temperature due the relatively high binding energy of this shallow trap. Trapping at these negative ions produces (S, W) parameters of the lattice and limits the effect of the trapping to cation vacancies on the annihilation parameters.…”
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