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Electroluminescent characteristics of InGaAsSb/GaAlAsSb heterostructure Mid-IR LEDs at high temperatures
The electroluminescent characteristics of an InGaAsSb/GaAlAsSb heterostructure LED emitting at 1.85 μm are studied in the temperature range 20–200°C. It is shown that the emission power exponentially drops as P ≅ 0.4exp(2.05 × 10 3 / T ) with a rise in temperature primarily because of an increase in...
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Published in: | Technical physics 2011-04, Vol.56 (4), p.520-525 |
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creator | Petukhov, A. A. Zhurtanov, B. E. Molchanov, S. S. Stoyanov, N. D. Yakovlev, Yu. P. |
description | The electroluminescent characteristics of an InGaAsSb/GaAlAsSb heterostructure LED emitting at 1.85 μm are studied in the temperature range 20–200°C. It is shown that the emission power exponentially drops as
P
≅ 0.4exp(2.05 × 10
3
/
T
) with a rise in temperature primarily because of an increase in the Auger recombination rate. It is found that band-to-band radiative recombination goes in parallel with recombination through acceptor levels, the latter causing the emission spectrum to broaden. With a rise in temperature, the activation energy of the acceptor levels decreases by the law Δ
E
≅ 32.9 − 0.075
T
and the maximum of the LED’s emission spectrum shifts toward the long-wavelength range (
hν
max
= 0.693 − 4.497 × 10
−4
T
). Based on the dependence
E
g
=
hν
max
− 0.5
kT
and experimental data, an expression is derived for the temperature variation of the bandgap in the In
0.055
Ga
0.945
AsSb active area,
E
g
≅ 0.817 − 4.951 × 10
−4
T
, in the range 290 K <
T
< 495 K. The resistance of the heterostructure decreases exponentially with rising temperature as
R
0
≅ 5.52 × 10
−2
exp(0.672/2
kT
), while cutoff voltage
U
cut
characterizing the barrier height of a
p−n
junction decreases linearly with increasing temperature (
U
cut
= −1.59
T
+ 534). It is found that the current through the heterostructure is due to the generation-recombination mechanism throughout the temperature interval. |
doi_str_mv | 10.1134/S1063784211040232 |
format | article |
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P
≅ 0.4exp(2.05 × 10
3
/
T
) with a rise in temperature primarily because of an increase in the Auger recombination rate. It is found that band-to-band radiative recombination goes in parallel with recombination through acceptor levels, the latter causing the emission spectrum to broaden. With a rise in temperature, the activation energy of the acceptor levels decreases by the law Δ
E
≅ 32.9 − 0.075
T
and the maximum of the LED’s emission spectrum shifts toward the long-wavelength range (
hν
max
= 0.693 − 4.497 × 10
−4
T
). Based on the dependence
E
g
=
hν
max
− 0.5
kT
and experimental data, an expression is derived for the temperature variation of the bandgap in the In
0.055
Ga
0.945
AsSb active area,
E
g
≅ 0.817 − 4.951 × 10
−4
T
, in the range 290 K <
T
< 495 K. The resistance of the heterostructure decreases exponentially with rising temperature as
R
0
≅ 5.52 × 10
−2
exp(0.672/2
kT
), while cutoff voltage
U
cut
characterizing the barrier height of a
p−n
junction decreases linearly with increasing temperature (
U
cut
= −1.59
T
+ 534). It is found that the current through the heterostructure is due to the generation-recombination mechanism throughout the temperature interval.</description><identifier>ISSN: 1063-7842</identifier><identifier>EISSN: 1090-6525</identifier><identifier>DOI: 10.1134/S1063784211040232</identifier><language>eng</language><publisher>Dordrecht: SP MAIK Nauka/Interperiodica</publisher><subject>Activation energy ; Classical and Continuum Physics ; Laws, regulations and rules ; Light-emitting diodes ; Optics ; Physics ; Physics and Astronomy ; Quantum Electronics ; Toy industry</subject><ispartof>Technical physics, 2011-04, Vol.56 (4), p.520-525</ispartof><rights>Pleiades Publishing, Ltd. 2011</rights><rights>COPYRIGHT 2011 Springer</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c327t-1454a476be29a453849a435b771244705323ab9d87d2a7990b3f906cd18f28263</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Petukhov, A. A.</creatorcontrib><creatorcontrib>Zhurtanov, B. E.</creatorcontrib><creatorcontrib>Molchanov, S. S.</creatorcontrib><creatorcontrib>Stoyanov, N. D.</creatorcontrib><creatorcontrib>Yakovlev, Yu. P.</creatorcontrib><title>Electroluminescent characteristics of InGaAsSb/GaAlAsSb heterostructure Mid-IR LEDs at high temperatures</title><title>Technical physics</title><addtitle>Tech. Phys</addtitle><description>The electroluminescent characteristics of an InGaAsSb/GaAlAsSb heterostructure LED emitting at 1.85 μm are studied in the temperature range 20–200°C. It is shown that the emission power exponentially drops as
P
≅ 0.4exp(2.05 × 10
3
/
T
) with a rise in temperature primarily because of an increase in the Auger recombination rate. It is found that band-to-band radiative recombination goes in parallel with recombination through acceptor levels, the latter causing the emission spectrum to broaden. With a rise in temperature, the activation energy of the acceptor levels decreases by the law Δ
E
≅ 32.9 − 0.075
T
and the maximum of the LED’s emission spectrum shifts toward the long-wavelength range (
hν
max
= 0.693 − 4.497 × 10
−4
T
). Based on the dependence
E
g
=
hν
max
− 0.5
kT
and experimental data, an expression is derived for the temperature variation of the bandgap in the In
0.055
Ga
0.945
AsSb active area,
E
g
≅ 0.817 − 4.951 × 10
−4
T
, in the range 290 K <
T
< 495 K. The resistance of the heterostructure decreases exponentially with rising temperature as
R
0
≅ 5.52 × 10
−2
exp(0.672/2
kT
), while cutoff voltage
U
cut
characterizing the barrier height of a
p−n
junction decreases linearly with increasing temperature (
U
cut
= −1.59
T
+ 534). It is found that the current through the heterostructure is due to the generation-recombination mechanism throughout the temperature interval.</description><subject>Activation energy</subject><subject>Classical and Continuum Physics</subject><subject>Laws, regulations and rules</subject><subject>Light-emitting diodes</subject><subject>Optics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Electronics</subject><subject>Toy industry</subject><issn>1063-7842</issn><issn>1090-6525</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp9kE1OwzAQhS0EEqVwAHa-QFqP7djJsiqlVCpCorCOHMdpXOWnsp0Ft8eh7JDQLN5oZr6R3kPoEcgCgPHlAYhgMuMUgHBCGb1CMyA5SURK0-upFyyZ9rfozvsTIQBZKmao2bRGBze0Y2d747XpA9aNckoH46wPVns81HjXb9XKH8pllHZqcGPiweCDG3UYncGvtkp273i_efJYBdzYY4OD6c7GqWnv79FNrVpvHn51jj6fNx_rl2T_tt2tV_tEMypDAjzliktRGpornrKMR2FpKSVQziVJGWWqzKtMVlTJPCclq3MidAVZTTMq2BwtLn-PqjWF7eshRDOxKtNZPfSmtnG-YoKIjMAPABdARzvembo4O9sp91UAKaZsiz_ZRoZeGB9v-6NxxWkYXR99_QN9AwGmejg</recordid><startdate>20110401</startdate><enddate>20110401</enddate><creator>Petukhov, A. A.</creator><creator>Zhurtanov, B. E.</creator><creator>Molchanov, S. S.</creator><creator>Stoyanov, N. D.</creator><creator>Yakovlev, Yu. P.</creator><general>SP MAIK Nauka/Interperiodica</general><general>Springer</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20110401</creationdate><title>Electroluminescent characteristics of InGaAsSb/GaAlAsSb heterostructure Mid-IR LEDs at high temperatures</title><author>Petukhov, A. A. ; Zhurtanov, B. E. ; Molchanov, S. S. ; Stoyanov, N. D. ; Yakovlev, Yu. P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c327t-1454a476be29a453849a435b771244705323ab9d87d2a7990b3f906cd18f28263</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Activation energy</topic><topic>Classical and Continuum Physics</topic><topic>Laws, regulations and rules</topic><topic>Light-emitting diodes</topic><topic>Optics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Electronics</topic><topic>Toy industry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Petukhov, A. A.</creatorcontrib><creatorcontrib>Zhurtanov, B. E.</creatorcontrib><creatorcontrib>Molchanov, S. S.</creatorcontrib><creatorcontrib>Stoyanov, N. D.</creatorcontrib><creatorcontrib>Yakovlev, Yu. P.</creatorcontrib><collection>CrossRef</collection><jtitle>Technical physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Petukhov, A. A.</au><au>Zhurtanov, B. E.</au><au>Molchanov, S. S.</au><au>Stoyanov, N. D.</au><au>Yakovlev, Yu. P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electroluminescent characteristics of InGaAsSb/GaAlAsSb heterostructure Mid-IR LEDs at high temperatures</atitle><jtitle>Technical physics</jtitle><stitle>Tech. Phys</stitle><date>2011-04-01</date><risdate>2011</risdate><volume>56</volume><issue>4</issue><spage>520</spage><epage>525</epage><pages>520-525</pages><issn>1063-7842</issn><eissn>1090-6525</eissn><abstract>The electroluminescent characteristics of an InGaAsSb/GaAlAsSb heterostructure LED emitting at 1.85 μm are studied in the temperature range 20–200°C. It is shown that the emission power exponentially drops as
P
≅ 0.4exp(2.05 × 10
3
/
T
) with a rise in temperature primarily because of an increase in the Auger recombination rate. It is found that band-to-band radiative recombination goes in parallel with recombination through acceptor levels, the latter causing the emission spectrum to broaden. With a rise in temperature, the activation energy of the acceptor levels decreases by the law Δ
E
≅ 32.9 − 0.075
T
and the maximum of the LED’s emission spectrum shifts toward the long-wavelength range (
hν
max
= 0.693 − 4.497 × 10
−4
T
). Based on the dependence
E
g
=
hν
max
− 0.5
kT
and experimental data, an expression is derived for the temperature variation of the bandgap in the In
0.055
Ga
0.945
AsSb active area,
E
g
≅ 0.817 − 4.951 × 10
−4
T
, in the range 290 K <
T
< 495 K. The resistance of the heterostructure decreases exponentially with rising temperature as
R
0
≅ 5.52 × 10
−2
exp(0.672/2
kT
), while cutoff voltage
U
cut
characterizing the barrier height of a
p−n
junction decreases linearly with increasing temperature (
U
cut
= −1.59
T
+ 534). It is found that the current through the heterostructure is due to the generation-recombination mechanism throughout the temperature interval.</abstract><cop>Dordrecht</cop><pub>SP MAIK Nauka/Interperiodica</pub><doi>10.1134/S1063784211040232</doi><tpages>6</tpages></addata></record> |
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source | Springer Link |
subjects | Activation energy Classical and Continuum Physics Laws, regulations and rules Light-emitting diodes Optics Physics Physics and Astronomy Quantum Electronics Toy industry |
title | Electroluminescent characteristics of InGaAsSb/GaAlAsSb heterostructure Mid-IR LEDs at high temperatures |
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