Effect of thin emitter set-back layer on GaAs delta-doped emitter bipolar junction transistor
GaAs delta-doped emitter bipolar junction transistors ( δ - BJT ) with different emitter set-back layer thicknesses of 10 to 50 nm were fabricated to study the emitter set-back layer thickness effect on device dc performance. We found that the current gain decreases following decrease in the emitter...
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creator | Lew, K. L. Yoon, S. F. |
description | GaAs delta-doped emitter bipolar junction transistors
(
δ
-
BJT
)
with different emitter set-back layer thicknesses of
10
to
50
nm
were fabricated to study the emitter set-back layer thickness effect on device dc performance. We found that the current gain decreases following decrease in the emitter set-back layer thickness. A detailed analysis was performed to explain this phenomenon, which is believed to be caused by reduction of the effective barrier height in the
δ
-
BJT
. This is due to change in the electric-field distribution in the delta-doped structure caused by the built-in potential of the base-emitter
(
B
-
E
)
junction. Considering the recombination and barrier height reduction effects, the thickness of the emitter set-back layer should be designed according to the
B
-
E
junction depletion width with a tolerance of
±
5
nm
. The dc performance of a
δ
-
BJT
designed based on this criteria is compared to that of a
Al
0.25
Ga
0.75
As
∕
Ga
As
heterojunction bipolar transistor (HBT). Both devices employed base doping of
2
×
10
19
cm
−
3
and base-to-emitter doping ratio of 40. Large emitter area
(
A
E
≈
1.6
×
10
−
5
cm
−
2
)
and small emitter area
(
A
E
≈
1.35
×
10
−
6
cm
−
2
)
device current gains of 40 and 20, respectively, were obtained in both types of transistors passivated by
(
N
H
4
)
2
S
treatment. The measured current gain of the GaAs
δ
-
BJT
is the highest reported for a homojunction device with such high base-to-emitter doping ratio normally used in HBT devices. |
doi_str_mv | 10.1063/1.1888049 |
format | Article |
fullrecord | <record><control><sourceid>scitation_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1063_1_1888049</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>jap</sourcerecordid><originalsourceid>FETCH-LOGICAL-c244t-4ce047eb0fd87afd5db2e659f846cf9c506bec9309b429dc00329cd8e8441dba3</originalsourceid><addsrcrecordid>eNp1kEtLAzEUhYMoWKsL_0G2LlJvZjIzyUYopVah4EaXEvLE1OmkJHHRf-_0gTtXlwMfh3M_hO4pzCi09SOdUc45MHGBJhS4IF3TwCWaAFSUcNGJa3ST8waAUl6LCfpceu9MwdHj8hUG7LahFJdwdoVoZb5xr_ZjjANeqXnG1vVFERt3zv6hOuxirxLe_AymhJEsSQ055BLTLbryqs_u7nyn6ON5-b54Ieu31etiviamYqwQZhywzmnwlnfK28bqyrWN8Jy1xgvTQKudETUIzSphDUBdCWO544xRq1U9RQ-nXpNizsl5uUthq9JeUpAHL5LKs5eRfTqx2YSiDoP_h09yZPTyIEceP65_AYCybCU</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Effect of thin emitter set-back layer on GaAs delta-doped emitter bipolar junction transistor</title><source>AIP Journals Complete</source><source>AIP Digital Archive</source><creator>Lew, K. L. ; Yoon, S. F.</creator><creatorcontrib>Lew, K. L. ; Yoon, S. F.</creatorcontrib><description>GaAs delta-doped emitter bipolar junction transistors
(
δ
-
BJT
)
with different emitter set-back layer thicknesses of
10
to
50
nm
were fabricated to study the emitter set-back layer thickness effect on device dc performance. We found that the current gain decreases following decrease in the emitter set-back layer thickness. A detailed analysis was performed to explain this phenomenon, which is believed to be caused by reduction of the effective barrier height in the
δ
-
BJT
. This is due to change in the electric-field distribution in the delta-doped structure caused by the built-in potential of the base-emitter
(
B
-
E
)
junction. Considering the recombination and barrier height reduction effects, the thickness of the emitter set-back layer should be designed according to the
B
-
E
junction depletion width with a tolerance of
±
5
nm
. The dc performance of a
δ
-
BJT
designed based on this criteria is compared to that of a
Al
0.25
Ga
0.75
As
∕
Ga
As
heterojunction bipolar transistor (HBT). Both devices employed base doping of
2
×
10
19
cm
−
3
and base-to-emitter doping ratio of 40. Large emitter area
(
A
E
≈
1.6
×
10
−
5
cm
−
2
)
and small emitter area
(
A
E
≈
1.35
×
10
−
6
cm
−
2
)
device current gains of 40 and 20, respectively, were obtained in both types of transistors passivated by
(
N
H
4
)
2
S
treatment. The measured current gain of the GaAs
δ
-
BJT
is the highest reported for a homojunction device with such high base-to-emitter doping ratio normally used in HBT devices.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.1888049</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>American Institute of Physics</publisher><ispartof>Journal of applied physics, 2005-05, Vol.97 (10), p.104502-104502-5</ispartof><rights>2005 American Institute of Physics</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c244t-4ce047eb0fd87afd5db2e659f846cf9c506bec9309b429dc00329cd8e8441dba3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/jap/article-lookup/doi/10.1063/1.1888049$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,1559,4512,27924,27925,76384,76390</link.rule.ids></links><search><creatorcontrib>Lew, K. L.</creatorcontrib><creatorcontrib>Yoon, S. F.</creatorcontrib><title>Effect of thin emitter set-back layer on GaAs delta-doped emitter bipolar junction transistor</title><title>Journal of applied physics</title><description>GaAs delta-doped emitter bipolar junction transistors
(
δ
-
BJT
)
with different emitter set-back layer thicknesses of
10
to
50
nm
were fabricated to study the emitter set-back layer thickness effect on device dc performance. We found that the current gain decreases following decrease in the emitter set-back layer thickness. A detailed analysis was performed to explain this phenomenon, which is believed to be caused by reduction of the effective barrier height in the
δ
-
BJT
. This is due to change in the electric-field distribution in the delta-doped structure caused by the built-in potential of the base-emitter
(
B
-
E
)
junction. Considering the recombination and barrier height reduction effects, the thickness of the emitter set-back layer should be designed according to the
B
-
E
junction depletion width with a tolerance of
±
5
nm
. The dc performance of a
δ
-
BJT
designed based on this criteria is compared to that of a
Al
0.25
Ga
0.75
As
∕
Ga
As
heterojunction bipolar transistor (HBT). Both devices employed base doping of
2
×
10
19
cm
−
3
and base-to-emitter doping ratio of 40. Large emitter area
(
A
E
≈
1.6
×
10
−
5
cm
−
2
)
and small emitter area
(
A
E
≈
1.35
×
10
−
6
cm
−
2
)
device current gains of 40 and 20, respectively, were obtained in both types of transistors passivated by
(
N
H
4
)
2
S
treatment. The measured current gain of the GaAs
δ
-
BJT
is the highest reported for a homojunction device with such high base-to-emitter doping ratio normally used in HBT devices.</description><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><recordid>eNp1kEtLAzEUhYMoWKsL_0G2LlJvZjIzyUYopVah4EaXEvLE1OmkJHHRf-_0gTtXlwMfh3M_hO4pzCi09SOdUc45MHGBJhS4IF3TwCWaAFSUcNGJa3ST8waAUl6LCfpceu9MwdHj8hUG7LahFJdwdoVoZb5xr_ZjjANeqXnG1vVFERt3zv6hOuxirxLe_AymhJEsSQ055BLTLbryqs_u7nyn6ON5-b54Ieu31etiviamYqwQZhywzmnwlnfK28bqyrWN8Jy1xgvTQKudETUIzSphDUBdCWO544xRq1U9RQ-nXpNizsl5uUthq9JeUpAHL5LKs5eRfTqx2YSiDoP_h09yZPTyIEceP65_AYCybCU</recordid><startdate>20050515</startdate><enddate>20050515</enddate><creator>Lew, K. L.</creator><creator>Yoon, S. F.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20050515</creationdate><title>Effect of thin emitter set-back layer on GaAs delta-doped emitter bipolar junction transistor</title><author>Lew, K. L. ; Yoon, S. F.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c244t-4ce047eb0fd87afd5db2e659f846cf9c506bec9309b429dc00329cd8e8441dba3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2005</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lew, K. L.</creatorcontrib><creatorcontrib>Yoon, S. F.</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lew, K. L.</au><au>Yoon, S. F.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of thin emitter set-back layer on GaAs delta-doped emitter bipolar junction transistor</atitle><jtitle>Journal of applied physics</jtitle><date>2005-05-15</date><risdate>2005</risdate><volume>97</volume><issue>10</issue><spage>104502</spage><epage>104502-5</epage><pages>104502-104502-5</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>GaAs delta-doped emitter bipolar junction transistors
(
δ
-
BJT
)
with different emitter set-back layer thicknesses of
10
to
50
nm
were fabricated to study the emitter set-back layer thickness effect on device dc performance. We found that the current gain decreases following decrease in the emitter set-back layer thickness. A detailed analysis was performed to explain this phenomenon, which is believed to be caused by reduction of the effective barrier height in the
δ
-
BJT
. This is due to change in the electric-field distribution in the delta-doped structure caused by the built-in potential of the base-emitter
(
B
-
E
)
junction. Considering the recombination and barrier height reduction effects, the thickness of the emitter set-back layer should be designed according to the
B
-
E
junction depletion width with a tolerance of
±
5
nm
. The dc performance of a
δ
-
BJT
designed based on this criteria is compared to that of a
Al
0.25
Ga
0.75
As
∕
Ga
As
heterojunction bipolar transistor (HBT). Both devices employed base doping of
2
×
10
19
cm
−
3
and base-to-emitter doping ratio of 40. Large emitter area
(
A
E
≈
1.6
×
10
−
5
cm
−
2
)
and small emitter area
(
A
E
≈
1.35
×
10
−
6
cm
−
2
)
device current gains of 40 and 20, respectively, were obtained in both types of transistors passivated by
(
N
H
4
)
2
S
treatment. The measured current gain of the GaAs
δ
-
BJT
is the highest reported for a homojunction device with such high base-to-emitter doping ratio normally used in HBT devices.</abstract><pub>American Institute of Physics</pub><doi>10.1063/1.1888049</doi></addata></record> |
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identifier | ISSN: 0021-8979 |
ispartof | Journal of applied physics, 2005-05, Vol.97 (10), p.104502-104502-5 |
issn | 0021-8979 1089-7550 |
language | eng |
recordid | cdi_crossref_primary_10_1063_1_1888049 |
source | AIP Journals Complete; AIP Digital Archive |
title | Effect of thin emitter set-back layer on GaAs delta-doped emitter bipolar junction transistor |
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