2017
DOI: 10.1021/acs.nanolett.7b01766
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Sub-Poissonian Narrowing of Length Distributions Realized in Ga-Catalyzed GaAs Nanowires

Abstract: Herein, we present experimental data on the record length uniformity within the ensembles of semiconductor nanowires. The length distributions of Ga-catalyzed GaAs nanowires obtained by cost-effective lithography-free technique on silicon substrates systematically feature a pronounced sub-Poissonian character. For example, nanowires with the mean length ⟨L⟩ of 2480 nm show a length distribution variance of only 367 nm, which is more than twice smaller than the Poisson variance h⟨L⟩ of 808 nm for this mean leng… Show more

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Cited by 42 publications
(75 citation statements)
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“…Self‐catalyzed vapor–liquid–solid (VLS) growth of III–V nanowires (NWs) is a promising gold‐free method for synthesis of high crystal quality and size‐uniform ensembles of NWs. Most self‐catalyzed III–V NWs are grown by molecular beam epitaxy (MBE) in regular arrays on lithographically patterned SiO x /Si(111) substrates with gallium predeposition, or using other methods of gallium droplet organization . Recently, sub‐Poissonian narrowing of the length distributions has been demonstrated for gallium‐catalyzed GaAs NWs .…”
Section: Parameters Of Gaas Nws Used In Calculationsmentioning
confidence: 99%
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“…Self‐catalyzed vapor–liquid–solid (VLS) growth of III–V nanowires (NWs) is a promising gold‐free method for synthesis of high crystal quality and size‐uniform ensembles of NWs. Most self‐catalyzed III–V NWs are grown by molecular beam epitaxy (MBE) in regular arrays on lithographically patterned SiO x /Si(111) substrates with gallium predeposition, or using other methods of gallium droplet organization . Recently, sub‐Poissonian narrowing of the length distributions has been demonstrated for gallium‐catalyzed GaAs NWs .…”
Section: Parameters Of Gaas Nws Used In Calculationsmentioning
confidence: 99%
“…The ρ function is given by ρ = 2 λ 3 sin α π χ ( α , β ) ( F 53 1 ) ( 1 θ lf ) [ cosh ( L / λ 3 ) 1 ] + θ sf θ lf sinh ( L / λ 3 ) and generally depends on α , β , F 53 , L false/ λ 3 , and λ 3 . The collection length λ 3 may be limited by the shadowing effect in MBE, with the trivial shadowing length related to the array pitch P and the beam angle α as λ 3 = P cot a n α . The value of ρ is very large for short NWs due to the additional collection of gallium adatoms from the smooth oxide surface, whereas, for long NWs with L false/ λ f 1 , it saturates to the length‐independent value ρ = 2 λ 3 sin α false( 1 θ lf false) false/ false[ π χ false( α , β false) false( F 53 1 false) false] .…”
Section: Parameters Of Gaas Nws Used In Calculationsmentioning
confidence: 99%
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