Serveur d'exploration sur l'Indium

Attention, ce site est en cours de développement !
Attention, site généré par des moyens informatiques à partir de corpus bruts.
Les informations ne sont donc pas validées.

Studies and comparisons of a N+-InGaP/δ(P+)-InGaP/n-GaAs hetero-planar-doped structure to high-linearity microwave field-effect transistors

Identifieur interne : 010898 ( Main/Repository ); précédent : 010897; suivant : 010899

Studies and comparisons of a N+-InGaP/δ(P+)-InGaP/n-GaAs hetero-planar-doped structure to high-linearity microwave field-effect transistors

Auteurs : RBID : Pascal:01-0206593

Descripteurs français

English descriptors

Abstract

We report a promising N+-InGaP/δ(P+)-InGaP/n-GaAs hetero-planar-doped barrier, which is used to fabricate both high-breakdown and self-aligned T-gate (SAT-gate) field-effect transistors (FETs). The characteristics of the devices and comparisons with previous reports are discussed. The enhanced conduction- and valence-band offsets associated with the new hetero-planar doped barrier show high-breakdown behaviour. In addition, high selective etching between InGaP and GaAs layers together with an ohmic gate allows the fabrication of a SAT-gate with a reduced gate-length of 0.8 μm. In the case of a high-breakdown FET, the drain-source breakdown voltage is as high as 32 V. In addition to competitive direct-current (dc) performances, a reduced knee voltage and improved frequency performances are obtained in SAT-gate FETs. The available unity-current-gain and unity-power-gain frequencies are, respectively, 19.5 and 30 GHz achieved as a 0.6 μm gate is obtained by forming a 1 μm metal gate. Furthermore, all the measured SAT-gate FETs exhibit high-linearity and high-uniformity dc and alternating-current performances.

Links toward previous steps (curation, corpus...)


Links to Exploration step

Pascal:01-0206593

Le document en format XML

<record>
<TEI>
<teiHeader>
<fileDesc>
<titleStmt>
<title xml:lang="en" level="a">Studies and comparisons of a N
<sup>+</sup>
-InGaP/δ(P
<sup>+</sup>
)-InGaP/n-GaAs hetero-planar-doped structure to high-linearity microwave field-effect transistors</title>
<author>
<name sortKey="Lour, W S" uniqKey="Lour W">W. S. Lour</name>
<affiliation wicri:level="1">
<inist:fA14 i1="01">
<s1>Department of Electrical Engineering, National Taiwan-Ocean University, No 2, Peining Road</s1>
<s2>Keelung</s2>
<s3>TWN</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Taïwan</country>
<wicri:noRegion>Keelung</wicri:noRegion>
</affiliation>
</author>
<author>
<name sortKey="Tsai, M K" uniqKey="Tsai M">M. K. Tsai</name>
<affiliation wicri:level="1">
<inist:fA14 i1="02">
<s1>Department of Electrical Engineering, National Taiwan University, No 1 Sec. 4, Roosevelt, Road</s1>
<s2>Taipei</s2>
<s3>TWN</s3>
<sZ>2 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>Taïwan</country>
<wicri:noRegion>Taipei</wicri:noRegion>
</affiliation>
</author>
<author>
<name sortKey="Lai, K Y" uniqKey="Lai K">K. Y. Lai</name>
<affiliation wicri:level="1">
<inist:fA14 i1="01">
<s1>Department of Electrical Engineering, National Taiwan-Ocean University, No 2, Peining Road</s1>
<s2>Keelung</s2>
<s3>TWN</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Taïwan</country>
<wicri:noRegion>Keelung</wicri:noRegion>
</affiliation>
</author>
<author>
<name sortKey="Chen, B L" uniqKey="Chen B">B. L. Chen</name>
<affiliation wicri:level="1">
<inist:fA14 i1="01">
<s1>Department of Electrical Engineering, National Taiwan-Ocean University, No 2, Peining Road</s1>
<s2>Keelung</s2>
<s3>TWN</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</inist:fA14>
<country>Taïwan</country>
<wicri:noRegion>Keelung</wicri:noRegion>
</affiliation>
</author>
<author>
<name sortKey="Yang, Y J" uniqKey="Yang Y">Y. J. Yang</name>
<affiliation wicri:level="1">
<inist:fA14 i1="02">
<s1>Department of Electrical Engineering, National Taiwan University, No 1 Sec. 4, Roosevelt, Road</s1>
<s2>Taipei</s2>
<s3>TWN</s3>
<sZ>2 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>Taïwan</country>
<wicri:noRegion>Taipei</wicri:noRegion>
</affiliation>
</author>
</titleStmt>
<publicationStmt>
<idno type="inist">01-0206593</idno>
<date when="2001">2001</date>
<idno type="stanalyst">PASCAL 01-0206593 INIST</idno>
<idno type="RBID">Pascal:01-0206593</idno>
<idno type="wicri:Area/Main/Corpus">011372</idno>
<idno type="wicri:Area/Main/Repository">010898</idno>
</publicationStmt>
<seriesStmt>
<idno type="ISSN">0268-1242</idno>
<title level="j" type="abbreviated">Semicond. sci. technol.</title>
<title level="j" type="main">Semiconductor science and technology</title>
</seriesStmt>
</fileDesc>
<profileDesc>
<textClass>
<keywords scheme="KwdEn" xml:lang="en">
<term>Band offset</term>
<term>Binary compound</term>
<term>Electrical characteristic</term>
<term>Gallium arsenides</term>
<term>Gallium phosphide</term>
<term>Gates</term>
<term>Heterojunctions</term>
<term>Indium phosphide</term>
<term>Microwave field effect transistors</term>
<term>Planar doping</term>
<term>Selective etching</term>
<term>Self aligned technology</term>
<term>Ternary compound</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Transistor effet champ hyperfréquence</term>
<term>Hétérojonction</term>
<term>Discontinuité bande</term>
<term>Dopage plan</term>
<term>Gravure sélective</term>
<term>Technologie autoalignée</term>
<term>Electrode commande</term>
<term>Caractéristique électrique</term>
<term>Gallium phosphure</term>
<term>Indium phosphure</term>
<term>Gallium arséniure</term>
<term>Composé binaire</term>
<term>Composé ternaire</term>
<term>Ga In P</term>
<term>InGaP</term>
<term>As Ga</term>
<term>GaAs</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front>
<div type="abstract" xml:lang="en">We report a promising N
<sup>+</sup>
-InGaP/δ(P
<sup>+</sup>
)-InGaP/n-GaAs hetero-planar-doped barrier, which is used to fabricate both high-breakdown and self-aligned T-gate (SAT-gate) field-effect transistors (FETs). The characteristics of the devices and comparisons with previous reports are discussed. The enhanced conduction- and valence-band offsets associated with the new hetero-planar doped barrier show high-breakdown behaviour. In addition, high selective etching between InGaP and GaAs layers together with an ohmic gate allows the fabrication of a SAT-gate with a reduced gate-length of 0.8 μm. In the case of a high-breakdown FET, the drain-source breakdown voltage is as high as 32 V. In addition to competitive direct-current (dc) performances, a reduced knee voltage and improved frequency performances are obtained in SAT-gate FETs. The available unity-current-gain and unity-power-gain frequencies are, respectively, 19.5 and 30 GHz achieved as a 0.6 μm gate is obtained by forming a 1 μm metal gate. Furthermore, all the measured SAT-gate FETs exhibit high-linearity and high-uniformity dc and alternating-current performances.</div>
</front>
</TEI>
<inist>
<standard h6="B">
<pA>
<fA01 i1="01" i2="1">
<s0>0268-1242</s0>
</fA01>
<fA02 i1="01">
<s0>SSTEET</s0>
</fA02>
<fA03 i2="1">
<s0>Semicond. sci. technol.</s0>
</fA03>
<fA05>
<s2>16</s2>
</fA05>
<fA06>
<s2>4</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG">
<s1>Studies and comparisons of a N
<sup>+</sup>
-InGaP/δ(P
<sup>+</sup>
)-InGaP/n-GaAs hetero-planar-doped structure to high-linearity microwave field-effect transistors</s1>
</fA08>
<fA11 i1="01" i2="1">
<s1>LOUR (W. S.)</s1>
</fA11>
<fA11 i1="02" i2="1">
<s1>TSAI (M. K.)</s1>
</fA11>
<fA11 i1="03" i2="1">
<s1>LAI (K. Y.)</s1>
</fA11>
<fA11 i1="04" i2="1">
<s1>CHEN (B. L.)</s1>
</fA11>
<fA11 i1="05" i2="1">
<s1>YANG (Y. J.)</s1>
</fA11>
<fA14 i1="01">
<s1>Department of Electrical Engineering, National Taiwan-Ocean University, No 2, Peining Road</s1>
<s2>Keelung</s2>
<s3>TWN</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="02">
<s1>Department of Electrical Engineering, National Taiwan University, No 1 Sec. 4, Roosevelt, Road</s1>
<s2>Taipei</s2>
<s3>TWN</s3>
<sZ>2 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14>
<fA20>
<s1>191-196</s1>
</fA20>
<fA21>
<s1>2001</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>21041</s2>
<s5>354000094519160020</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2001 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>9 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>01-0206593</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Semiconductor science and technology</s0>
</fA64>
<fA66 i1="01">
<s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>We report a promising N
<sup>+</sup>
-InGaP/δ(P
<sup>+</sup>
)-InGaP/n-GaAs hetero-planar-doped barrier, which is used to fabricate both high-breakdown and self-aligned T-gate (SAT-gate) field-effect transistors (FETs). The characteristics of the devices and comparisons with previous reports are discussed. The enhanced conduction- and valence-band offsets associated with the new hetero-planar doped barrier show high-breakdown behaviour. In addition, high selective etching between InGaP and GaAs layers together with an ohmic gate allows the fabrication of a SAT-gate with a reduced gate-length of 0.8 μm. In the case of a high-breakdown FET, the drain-source breakdown voltage is as high as 32 V. In addition to competitive direct-current (dc) performances, a reduced knee voltage and improved frequency performances are obtained in SAT-gate FETs. The available unity-current-gain and unity-power-gain frequencies are, respectively, 19.5 and 30 GHz achieved as a 0.6 μm gate is obtained by forming a 1 μm metal gate. Furthermore, all the measured SAT-gate FETs exhibit high-linearity and high-uniformity dc and alternating-current performances.</s0>
</fC01>
<fC02 i1="01" i2="X">
<s0>001D03F04</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Transistor effet champ hyperfréquence</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Microwave field effect transistors</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="1" l="FRE">
<s0>Hétérojonction</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="1" l="ENG">
<s0>Heterojunctions</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE">
<s0>Discontinuité bande</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG">
<s0>Band offset</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA">
<s0>Discontinuidad banda</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Dopage plan</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Planar doping</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Doping plano</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE">
<s0>Gravure sélective</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG">
<s0>Selective etching</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA">
<s0>Grabado selectivo</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Technologie autoalignée</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Self aligned technology</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Tecnología rejilla autoalineada</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Electrode commande</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Gates</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE">
<s0>Caractéristique électrique</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG">
<s0>Electrical characteristic</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA">
<s0>Característica eléctrica</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Gallium phosphure</s0>
<s5>23</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Gallium phosphide</s0>
<s5>23</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Galio fosfuro</s0>
<s5>23</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Indium phosphure</s0>
<s5>24</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>Indium phosphide</s0>
<s5>24</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Indio fosfuro</s0>
<s5>24</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Gallium arséniure</s0>
<s2>NK</s2>
<s5>26</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Gallium arsenides</s0>
<s2>NK</s2>
<s5>26</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE">
<s0>Composé binaire</s0>
<s5>27</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG">
<s0>Binary compound</s0>
<s5>27</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA">
<s0>Compuesto binario</s0>
<s5>27</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Composé ternaire</s0>
<s5>28</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>Ternary compound</s0>
<s5>28</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA">
<s0>Compuesto ternario</s0>
<s5>28</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE">
<s0>Ga In P</s0>
<s4>INC</s4>
<s5>82</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE">
<s0>InGaP</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE">
<s0>As Ga</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="17" i2="X" l="FRE">
<s0>GaAs</s0>
<s4>INC</s4>
<s5>85</s5>
</fC03>
<fN21>
<s1>141</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

Pour manipuler ce document sous Unix (Dilib)

EXPLOR_STEP=IndiumV3/Data/Main/Repository
HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 010898 | SxmlIndent | more

Ou

HfdSelect -h $EXPLOR_AREA/Data/Main/Repository/biblio.hfd -nk 010898 | SxmlIndent | more

Pour mettre un lien sur cette page dans le réseau Wicri

{{Explor lien
   |wiki=   *** parameter Area/wikiCode missing *** 
   |area=    IndiumV3
   |flux=    Main
   |étape=   Repository
   |type=    RBID
   |clé=     Pascal:01-0206593
   |texte=   Studies and comparisons of a N+-InGaP/δ(P+)-InGaP/n-GaAs hetero-planar-doped structure to high-linearity microwave field-effect transistors
}}

Wicri

This area was generated with Dilib version V0.5.77.
Data generation: Mon Jun 9 10:27:54 2014. Site generation: Thu Mar 7 16:19:59 2024