Abstract:Optical properties of wurtzite InP/InAs/InP core-shell nanowires grown on silicon substrates by solid source molecular beam epitaxy are studied by means of photoluminescence and microphotoluminescence. The growth conditions were optimized to obtain purely wurtzite radial quantum wells emitting in the telecom bands with a radiative lifetime in the 5-7 ns range at 14 K. Optical studies on single nanowires reveal that the polarization is mainly parallel to the growth direction. A 20-fold reduction of the photolum… Show more
“…It has been recently shown by a number of authors (see, e.g., Refs. [13][14][15][16]) that NWs of narrow-gap III-V semiconductors may not have a zinc-blende crystalline structure, as bulk crystals, but a wurtzite one. The high-resolution TEM microscopy showed 11 that in our samples the InAs base grows with the wurtzite structure, whereas the top InSb segment crystallizes in the zinc blende phase, which agrees with the results of other authors.…”
The electrical properties of nanowire-based n-InSb-n-InAs heterojunctions were investigated theoretically and experimentally. Analysis of the current-voltage characteristics showed that the current through the heterojunction is caused mostly by generation-recombination processes in the InSb and at the heterointerface. Due to the partially overlapping valence band of InSb and the conduction band of InAs, the second process is fast and activationless. Theoretical analysis showed that, depending on the heterojunction parameters, the flux of non-equilibrium minority carriers may have a different direction, explaining the experimentally observed non-monotonic coordinate dependence of the electron beam induced current
“…It has been recently shown by a number of authors (see, e.g., Refs. [13][14][15][16]) that NWs of narrow-gap III-V semiconductors may not have a zinc-blende crystalline structure, as bulk crystals, but a wurtzite one. The high-resolution TEM microscopy showed 11 that in our samples the InAs base grows with the wurtzite structure, whereas the top InSb segment crystallizes in the zinc blende phase, which agrees with the results of other authors.…”
The electrical properties of nanowire-based n-InSb-n-InAs heterojunctions were investigated theoretically and experimentally. Analysis of the current-voltage characteristics showed that the current through the heterojunction is caused mostly by generation-recombination processes in the InSb and at the heterointerface. Due to the partially overlapping valence band of InSb and the conduction band of InAs, the second process is fast and activationless. Theoretical analysis showed that, depending on the heterojunction parameters, the flux of non-equilibrium minority carriers may have a different direction, explaining the experimentally observed non-monotonic coordinate dependence of the electron beam induced current
“…Details concerning the growth parameters (growth temperature, V/III beam equivalent pressure ratio, growth rate) can be found elsewhere [25,26]. In order to grow Gd 2 O 3 , the InP NWs on Si substrate were then introduced into a separate MBE reactor equipped with an electron gun evaporator and a granular Gd 2 O 3 target.…”
Section: Methodsmentioning
confidence: 99%
“…InP NWs exhibit a wurtzite structure with the growth direction perpendicular to the (0002) InP WZ lattice plane [25,26]. The NWs facets are parallel to (1-100) planes.…”
“…Although nanowire heterostructures combining various materials have been extensively reported, [9][10][11][12][13][14][15][16][17][18][19][20] reports on the use of InP-InGaAs material combination in nanowires have been surprisingly rare. 12, [21][22][23][24][25] In fact, InP-InGaAs nanowire QWs have not been reported despite popularity of their planar counterpart.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore theoretically predicted values, ZB values, realistic estimations and linear interpolation are often used in most WZ calculations. 17,18 Here too, the same approach is adopted where appropriate. The blue curve in Fig It could be seen that once the material system and the structure is modelled, together with the relationship between growth time and QW thickness given in Fig.…”
Wurtzite phase InP–InxGa1−xAs nanowire radial quantum wells were grown for the first time, with tunable emission in the 1.3–1.55 μm optical communication wavelength range.
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