Abstract:Composition and carrier-concentration dependence of the electronic structure of In y Ga 1 − y As 1 − x N x films with nitrogen mole fraction of less than 0.012 J. Appl. Phys. 98, 093714 (2005); 10.1063/1.2127126Effect of lithium ion irradiation on the transport and optical properties of Bridgman grown n-type InSb single crystals
“…B is much lighter than Ga and possesses a higher electronegativity. Applying the electronegativity rule suggests that boron should form localized electronic states in GaP or GaAs that should act as electron traps in accordance with recent experiments [4,5]. Based on the results of these experiments and corresponding theoretical considerations, we assume that the energies of the boron localized states comprising isolated boron states, boron pairs, and higher cluster states vary linearly with composition y in (B,Ga)As y P -y 1 of low B content [6,7,9,10].…”
We study the magnetotransport properties of n-type B x Ga 1-x As 0.11 P 0.89 :Te alloy samples with x 0 0.038 in magnetic fields up to 4 T between 10 and 280 K, some samples also under hydrostatic pressure up to 15 kbar. As a general trend the resistivity increases with increasing x, as both the carrier concentration and the mobility of electrons decrease. The free carrier concentration and mobility of the reference sample GaAs 0.11 P 0.89 :Te is almost independent of the applied hydrostatic pressure, in particular, at higher temperatures whereas the B 0.018 Ga 0.982 As 0.11 P 0.89 :Te sample exhibits a different behavior. Its resistivity decreases due to a substantial increase of its free carrier concentration under pressure. This behavior is explained by the existence of a boron-related density of localized states in the vicinity of the conduction band edge of the alloy. The boron states act as electron traps as well as efficient scattering centers. Applying hydrostatic pressure shifts the energetic positions of conduction band edge at the X-point and of the boron states apart, reducing the impact of boron on the electronic transport properties of the alloy.
“…B is much lighter than Ga and possesses a higher electronegativity. Applying the electronegativity rule suggests that boron should form localized electronic states in GaP or GaAs that should act as electron traps in accordance with recent experiments [4,5]. Based on the results of these experiments and corresponding theoretical considerations, we assume that the energies of the boron localized states comprising isolated boron states, boron pairs, and higher cluster states vary linearly with composition y in (B,Ga)As y P -y 1 of low B content [6,7,9,10].…”
We study the magnetotransport properties of n-type B x Ga 1-x As 0.11 P 0.89 :Te alloy samples with x 0 0.038 in magnetic fields up to 4 T between 10 and 280 K, some samples also under hydrostatic pressure up to 15 kbar. As a general trend the resistivity increases with increasing x, as both the carrier concentration and the mobility of electrons decrease. The free carrier concentration and mobility of the reference sample GaAs 0.11 P 0.89 :Te is almost independent of the applied hydrostatic pressure, in particular, at higher temperatures whereas the B 0.018 Ga 0.982 As 0.11 P 0.89 :Te sample exhibits a different behavior. Its resistivity decreases due to a substantial increase of its free carrier concentration under pressure. This behavior is explained by the existence of a boron-related density of localized states in the vicinity of the conduction band edge of the alloy. The boron states act as electron traps as well as efficient scattering centers. Applying hydrostatic pressure shifts the energetic positions of conduction band edge at the X-point and of the boron states apart, reducing the impact of boron on the electronic transport properties of the alloy.
“…Magnetotransport measurements under hydrostatic pressure can provide an indication for the average B related density of states (DOS). [15][16][17] These measurements suggest that the states of isolated B atoms and B clusters, which can act as isovalent charge carrier traps, are located in the region of the CB. However, the interpretation of pressure dependent magnetotransport measurements is rather challenging due to a lack of structural information.…”
Section: This Implies That Optical Transitions Between the B States Amentioning
confidence: 93%
“…Under group V rich growth conditions, as used in the investigated sample, isovalent incorporation on cationic positions is strongly favored. [15][16][17] The covalent radius of B (r B ¼ 85 pm) is much smaller than the covalent radii of Ga (r Ga ¼ 124 pm) and As (r As ¼ 121 pm) in the surrounding matrix. 10 This means the covalent B-As bonds are shorter than the covalent Ga-As bonds, r B þ r As < r Ga þ r As , which locally deforms the surrounding GaAs matrix towards the B impurity.…”
Section: A Classification Of the Main Boron Related Featuresmentioning
confidence: 99%
“…This illustrates that the impurity state of a B atom in the {110} surfaces does not lie 0.3 eV above the CBE as suggested for bulk GaAs layers. 17 The spectral structure of the experimental dI=dUðU; rÞ curves is much more indicative of a B impurity state in the band gap slightly below the CB. It is not unusual that the {110} surface affects the energetic position of the dopants.…”
Section: B Boron Induced Modifications Of the Local Electronic Strucmentioning
confidence: 99%
“…This suggests that the extraordinary increase in the CB effective mass, which is reported for boride III-V semiconductors, may not be attributed to the B first nearest neighbor paring in the transition region between a dilute system and an alloy. 15,17,30 Further work is needed to clarify whether the observed deviations in the spatial B distribution from a CSRP in QWs 3 with a B concentration of 1% prevail also at lower and higher amounts of B atoms.…”
Section: Characterization Of the Spatial Boron Distributionmentioning
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