Abstract:Growth mode and structural properties of GaSb layers grown on silicon substrate by molecular beam epitaxy method are investigated by transmission electron microscopy. It is found that the GaSb grows to three-dimensional islands and grains are tilted to reduce a lattice mismatch through twin boundaries when they are directly grown on Si substrate. A low-temperature (LT) AlSb buffer plays a key role in transferring the growth mode from a three-dimensional island to a layer-by-layer structure. When the LT AlSb la… Show more
“…The IMF arrays have been reported in several systems including GaP/Si [9], GaAs/Si [10], InAs/GaAs [11], InAs/ GaP [12], GaSb/GaAs [14][15][16][17][18], InP/GaAs [21] and AlSb/Si [22,23] over a range of lattice-mismatched conditions ranging from Da o /a o ¼ 0.4% (GaP/Si) to Da o /a o $13% (AlSb/Si). To date, the IMF formation process has not been well established in the literature.…”
Section: Introductionmentioning
confidence: 99%
“…The latter approach involving IMF formation appears fundamentally different from the metamorphic approach as strain energy is immediately relieved at the interface by laterally propagating (901) misfit dislocations confined to the epi-substrate interface [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23]. After IMF array formation, subsequent material deposition proceeds in a strainfree layer-by-layer growth mode.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, lattice-mismatched epitaxy of Sb-based materials on GaAs and Si substrates are attractive for advanced optoelectronic devices including monolithically integrated lasers [1,2], detectors [3,4], solar cells [5,6] and transistors [7,8]. Two prominent approaches to mismatched epitaxy involve either thick monolithic buffer layers or interfacial misfit dislocation (IMF) arrays [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23]. The former growth technique involves tetragonal distortion within a critical thickness followed by misfit dislocation and often threading dislocations to alleviate strain in the bulk material [24].…”
“…The IMF arrays have been reported in several systems including GaP/Si [9], GaAs/Si [10], InAs/GaAs [11], InAs/ GaP [12], GaSb/GaAs [14][15][16][17][18], InP/GaAs [21] and AlSb/Si [22,23] over a range of lattice-mismatched conditions ranging from Da o /a o ¼ 0.4% (GaP/Si) to Da o /a o $13% (AlSb/Si). To date, the IMF formation process has not been well established in the literature.…”
Section: Introductionmentioning
confidence: 99%
“…The latter approach involving IMF formation appears fundamentally different from the metamorphic approach as strain energy is immediately relieved at the interface by laterally propagating (901) misfit dislocations confined to the epi-substrate interface [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23]. After IMF array formation, subsequent material deposition proceeds in a strainfree layer-by-layer growth mode.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, lattice-mismatched epitaxy of Sb-based materials on GaAs and Si substrates are attractive for advanced optoelectronic devices including monolithically integrated lasers [1,2], detectors [3,4], solar cells [5,6] and transistors [7,8]. Two prominent approaches to mismatched epitaxy involve either thick monolithic buffer layers or interfacial misfit dislocation (IMF) arrays [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23]. The former growth technique involves tetragonal distortion within a critical thickness followed by misfit dislocation and often threading dislocations to alleviate strain in the bulk material [24].…”
“…Since then the IMF has been implemented in several systems including GaP/Si [11], GaAs/Si [12], InAs/GaAs [13], InAs/GaP [14], InP/GaAs [15], AlSb/Si [16] and GaAs on GaSb [17]. However, so far this mode has not been well-established due to both unrepeatable growth under technological conditions in a narrow epitaxial window and complex characterization.…”
A comprehensive investigation of the interfacial misfit (IMF) array formation has been carried out. The studies were based on the static phase diagram for GaAs (001) surface and As 2 dimers on the surface. Prior to the initiation of the GaSb growth two attempts of the temperature decreasing were performed: before and after the GaAs termination. The GaAs was grown in the optimal conditions for GaSb material. The influence of the interruption time on GaSb/GaAs heterostructure parameters was examined. Two cases were investigated: with and without Sb-soaking of the GaAs surface. The periodic array of edge dislocations at GaSb/GaAs interface was confirmed using Burger's circuit theory. Careful examination of misfit surroundings revealed one uncompleted Burger's vector that indicated one dislocation of mixed type among eight of the edge type. The distance between lattice sites of dislocations was 5.51 nm on average. The crystal quality of 5.0 µm GaSb layer was characterized by FWHM 2θ/ω = 42 arcsec, FWHM RC = 125 arcsec. The EPD = 4 × 10 6 cm − 2 was estimated after etching in FeCl 3 :HCl solution. The Δq z /Δq x ratio of 0.60 for 5.0 µm GaSb layer was higher than for 2.5 µm GaSb layer of 0.59. The probable reason was the thickness-dependent 60° dislocation density. The electrical parameters measured for 2.5 µm GaSb were: p = 4.0 × 10 16 cm −3 (2.0 × 10 16 cm −3 ) and µ = 599 cm 2 /V s (3420 cm 2 /V s) at 300 K (77 K).
“…For the past few years, epitaxial growth and characterization of GaSb layers on Si have been reported by several workers [6][7][8]. Akahane et al [9][10][11] reported the heteroepitaxial growth of GaSb films on Si substrates by introducing an AlSb initiation layer.…”
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