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Volumn 95, Issue 8, 2009, Pages

Photocurrent and photoconductance properties of a GaAs nanowire

Author keywords

[No Author keywords available]

Indexed keywords

GAAS; LASER FIELDS; METAL SOURCES; PHOTOCONDUCTANCE; PHOTOCONDUCTANCE SIGNALS; SCHOTTKY CONTACTS;

EID: 69549110180     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3193540     Document Type: Article
Times cited : (89)

References (31)
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    • 2 -chiat room temperature. The maximum of the photoluminescence at EPL ∼1.43 eV agrees reasonably well with the band gaenergy EGaAs at room temperature.
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    • h = 102 is smaller than the number Nphoton of absorbed photons per cycle, which can be estimated as Nphoton = Ilaser A α d/ (Ephoton fchop) =30 μW/ cm2 × (2.8× 10-9 cm2) ×0.014/ (1.7 eV×930 Hz) ≈ 105, with A the illuminated area of the wire, d its thickness, and α the absorption coefficient of GaAs, thus enabling the discussed photodoping effect.
    • h = 102 is smaller than the number Nphoton of absorbed photons per cycle, which can be estimated as Nphoton = Ilaser A α d/ (Ephoton fchop) =30 μW/ cm2 × (2.8× 10-9 cm2) ×0.014/ (1.7 eV×930 Hz) ≈ 105, with A the illuminated area of the wire, d its thickness, and α the absorption coefficient of GaAs, thus enabling the discussed photodoping effect.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.