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Defect properties of InGaAsN layers grown as sub-monolayer digital alloys by molecular beam epitaxy.

Authors :
Baranov, Artem I.
Gudovskikh, Alexander S.
Kudryashov, Dmitry A.
Lazarenko, Alexandra A.
Morozov, Ivan A.
Mozharov, Alexey M.
Nikitina, Ekaterina V.
Pirogov, Evgeny V.
Sobolev, Maxim S.
Zelentsov, Kirill S.
Egorov, Anton Yu.
Darga, Arouna
Le Gall, Sylvain
Kleider, Jean-Paul
Source :
Journal of Applied Physics; 2018, Vol. 123 Issue 16, pN.PAG-N.PAG, 11p, 1 Diagram, 1 Chart, 10 Graphs
Publication Year :
2018

Abstract

The defect properties of InGaAsN dilute nitrides grown as sub-monolayer digital alloys (SDAs) by molecular beam epitaxy for photovoltaic application were studied by space charge capacitance spectroscopy. Alloys of i-InGaAsN (<italic>E<subscript>g</subscript></italic> = 1.03 eV) were lattice-matched grown on GaAs wafers as a superlattice of InAs/GaAsN with one monolayer of InAs (<0.5 nm) between wide GaAsN (7–12 nm) layers as active layers in single-junction solar cells. Low p-type background doping was demonstrated at room temperature in samples with InGaAsN layers 900 nm and 1200 nm thick (less 1 × 10<superscript>15</superscript> cm<superscript>−3</superscript>). According to admittance spectroscopy and deep-level transient spectroscopy measurements, the SDA approach leads to defect-free growth up to a thickness of 900 nm. An increase in thickness to 1200 nm leads to the formation of non-radiative recombination centers with an activation energy of 0.5 eV (<italic>N<subscript>T</subscript></italic> = 8.4 × 10<superscript>14</superscript> cm<superscript>−3</superscript>) and a shallow defect level at 0.20 eV. The last one leads to the appearance of additional doping, but its concentration is low (<italic>N<subscript>T</subscript></italic> = 5 × 10<superscript>14</superscript> cm<superscript>−3</superscript>) so it does not affect the photoelectric properties. However, further increase in thickness to 1600 nm, leads to significant growth of its concentration to (3–5) × 10<superscript>15</superscript> cm<superscript>−3</superscript>, while the concentration of deep levels becomes 1.3 × 10<superscript>15</superscript> cm<superscript>−3</superscript>. Therefore, additional free charge carriers appearing due to ionization of the shallow level change the band diagram from p-i-n to p-n junction at room temperature. It leads to a drop of the external quantum efficiency due to the effect of pulling electric field decrease in the p-n junction and an increased number of non-radiative recombination centers that negatively impact lifetimes in InGaAsN. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00218979
Volume :
123
Issue :
16
Database :
Complementary Index
Journal :
Journal of Applied Physics
Publication Type :
Academic Journal
Accession number :
129382327
Full Text :
https://doi.org/10.1063/1.5011371