300-GHz InAlN/GaN HEMTs With InGaN Back Barrier
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Abstract
This letter reports lattice-matched In0.17Al0.83N/ GaN high-electron-mobility transistors on a SiC substrate with a record current gain cutoff frequency ( fT) of 300 GHz. To suppress the short-channel effects (SCEs), an In0.15Ga0.85N back barrier is applied in an InAlN/GaN heterostructure for the first time. The GaN channel thickness is also scaled to 26 nm, which allows a good immunity to SCEs for gate lengths down to 70 nm even with a relatively thick top barrier (9.4-10.4 nm). In a 30-nm-gate-length device with an on-resistance (Ron) of 1.2 Ω . mm and an extrinsic transconductance (gm.ext) of 530 mS/mm, a peak fT of 300 GHz is achieved. An electron velocity of 1.37-1.45 × 107 cm/s is extracted by two different delay analysis methods.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">300-GHz InAlN/GaN HEMTs With InGaN Back Barrier</title>
<author><name>DONG SEUP LEE</name>
<affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Microsystems Technology Laboratories, Massachusetts Institute of Technology</s1>
<s2>Cambridge, MA 02139</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
<placeName><settlement type="city">Cambridge (Massachusetts)</settlement>
<region type="state">Massachusetts</region>
</placeName>
<orgName type="university">Massachusetts Institute of Technology</orgName>
</affiliation>
</author>
<author><name>XIANG GAO</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>IQE RF LLC</s1>
<s2>Somerset, NJ 08873</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
<wicri:noRegion>IQE RF LLC</wicri:noRegion>
</affiliation>
</author>
<author><name>SHIPING GUO</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>IQE RF LLC</s1>
<s2>Somerset, NJ 08873</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
<wicri:noRegion>IQE RF LLC</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Kopp, David" uniqKey="Kopp D">David Kopp</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Department of Electrical Engineering, University of Notre Dame</s1>
<s2>Notre Dame, IN 46556</s2>
<s3>USA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
<wicri:noRegion>Notre Dame, IN 46556</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Fay, Patrick" uniqKey="Fay P">Patrick Fay</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Department of Electrical Engineering, University of Notre Dame</s1>
<s2>Notre Dame, IN 46556</s2>
<s3>USA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
<wicri:noRegion>Notre Dame, IN 46556</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Palacios, Tomas" uniqKey="Palacios T">Tomas Palacios</name>
<affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Microsystems Technology Laboratories, Massachusetts Institute of Technology</s1>
<s2>Cambridge, MA 02139</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>États-Unis</country>
<placeName><settlement type="city">Cambridge (Massachusetts)</settlement>
<region type="state">Massachusetts</region>
</placeName>
<orgName type="university">Massachusetts Institute of Technology</orgName>
</affiliation>
</author>
</titleStmt>
<publicationStmt><idno type="inist">11-0505060</idno>
<date when="2011">2011</date>
<idno type="stanalyst">PASCAL 11-0505060 INIST</idno>
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<idno type="wicri:Area/Main/Corpus">002553</idno>
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<seriesStmt><idno type="ISSN">0741-3106</idno>
<title level="j" type="abbreviated">IEEE electron device lett.</title>
<title level="j" type="main">IEEE electron device letters</title>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Binary compound</term>
<term>Current gain</term>
<term>Cut off frequency</term>
<term>Delay time</term>
<term>Gallium nitride</term>
<term>Heterostructures</term>
<term>High electron mobility transistor</term>
<term>Indium nitride</term>
<term>Mismatch lattice</term>
<term>Short channel</term>
<term>Silicon carbide</term>
<term>Ternary compound</term>
<term>Transconductance</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Transistor mobilité électron élevée</term>
<term>Accommodation réseau</term>
<term>Gain courant</term>
<term>Fréquence coupure</term>
<term>Canal court</term>
<term>Hétérostructure</term>
<term>Transconductance</term>
<term>Temps retard</term>
<term>Nitrure de gallium</term>
<term>Composé binaire</term>
<term>Composé ternaire</term>
<term>Nitrure d'indium</term>
<term>Carbure de silicium</term>
<term>GaN</term>
<term>InGaN</term>
<term>SiC</term>
</keywords>
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</teiHeader>
<front><div type="abstract" xml:lang="en">This letter reports lattice-matched In<sub>0.17</sub>
Al<sub>0.83</sub>
N/ GaN high-electron-mobility transistors on a SiC substrate with a record current gain cutoff frequency ( <sub>f</sub>
T) of 300 GHz. To suppress the short-channel effects (SCEs), an In<sub>0.15</sub>
Ga<sub>0.85</sub>
N back barrier is applied in an InAlN/GaN heterostructure for the first time. The GaN channel thickness is also scaled to 26 nm, which allows a good immunity to SCEs for gate lengths down to 70 nm even with a relatively thick top barrier (9.4-10.4 nm). In a 30-nm-gate-length device with an on-resistance (R<sub>on</sub>
) of 1.2 Ω . mm and an extrinsic transconductance (g<sub>m.ext</sub>
) of 530 mS/mm, a peak f<sub>T</sub>
of 300 GHz is achieved. An electron velocity of 1.37-1.45 × 10<sup>7</sup>
cm/s is extracted by two different delay analysis methods.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0741-3106</s0>
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<fA02 i1="01"><s0>EDLEDZ</s0>
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<fA03 i2="1"><s0>IEEE electron device lett.</s0>
</fA03>
<fA05><s2>32</s2>
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<fA06><s2>11</s2>
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<fA08 i1="01" i2="1" l="ENG"><s1>300-GHz InAlN/GaN HEMTs With InGaN Back Barrier</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>DONG SEUP LEE</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>XIANG GAO</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>SHIPING GUO</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>KOPP (David)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>FAY (Patrick)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>PALACIOS (Tomas)</s1>
</fA11>
<fA14 i1="01"><s1>Microsystems Technology Laboratories, Massachusetts Institute of Technology</s1>
<s2>Cambridge, MA 02139</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>IQE RF LLC</s1>
<s2>Somerset, NJ 08873</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Department of Electrical Engineering, University of Notre Dame</s1>
<s2>Notre Dame, IN 46556</s2>
<s3>USA</s3>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
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<fA20><s1>1525-1527</s1>
</fA20>
<fA21><s1>2011</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>222V</s2>
<s5>354000505574470190</s5>
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<fA44><s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
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<fC01 i1="01" l="ENG"><s0>This letter reports lattice-matched In<sub>0.17</sub>
Al<sub>0.83</sub>
N/ GaN high-electron-mobility transistors on a SiC substrate with a record current gain cutoff frequency ( <sub>f</sub>
T) of 300 GHz. To suppress the short-channel effects (SCEs), an In<sub>0.15</sub>
Ga<sub>0.85</sub>
N back barrier is applied in an InAlN/GaN heterostructure for the first time. The GaN channel thickness is also scaled to 26 nm, which allows a good immunity to SCEs for gate lengths down to 70 nm even with a relatively thick top barrier (9.4-10.4 nm). In a 30-nm-gate-length device with an on-resistance (R<sub>on</sub>
) of 1.2 Ω . mm and an extrinsic transconductance (g<sub>m.ext</sub>
) of 530 mS/mm, a peak f<sub>T</sub>
of 300 GHz is achieved. An electron velocity of 1.37-1.45 × 10<sup>7</sup>
cm/s is extracted by two different delay analysis methods.</s0>
</fC01>
<fC02 i1="01" i2="X"><s0>001D03F04</s0>
</fC02>
<fC02 i1="02" i2="X"><s0>001D03F02</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Transistor mobilité électron élevée</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>High electron mobility transistor</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Transistor movibilidad elevada electrones</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Accommodation réseau</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG"><s0>Mismatch lattice</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA"><s0>Acomodación red</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE"><s0>Gain courant</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG"><s0>Current gain</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA"><s0>Ganancia corriente</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Fréquence coupure</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG"><s0>Cut off frequency</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA"><s0>Frecuencia corte</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Canal court</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Short channel</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Canal corto</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Hétérostructure</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Heterostructures</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Transconductance</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Transconductance</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Transconductancia</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Temps retard</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Delay time</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA"><s0>Tiempo retardo</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Nitrure de gallium</s0>
<s5>22</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Gallium nitride</s0>
<s5>22</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Galio nitruro</s0>
<s5>22</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Composé binaire</s0>
<s5>23</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Binary compound</s0>
<s5>23</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Compuesto binario</s0>
<s5>23</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE"><s0>Composé ternaire</s0>
<s5>24</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG"><s0>Ternary compound</s0>
<s5>24</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA"><s0>Compuesto ternario</s0>
<s5>24</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Nitrure d'indium</s0>
<s5>25</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>Indium nitride</s0>
<s5>25</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Indio nitruro</s0>
<s5>25</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE"><s0>Carbure de silicium</s0>
<s5>26</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG"><s0>Silicon carbide</s0>
<s5>26</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA"><s0>Silicio carburo</s0>
<s5>26</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>GaN</s0>
<s4>INC</s4>
<s5>82</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE"><s0>InGaN</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE"><s0>SiC</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC07 i1="01" i2="X" l="FRE"><s0>Composé III-V</s0>
<s5>09</s5>
</fC07>
<fC07 i1="01" i2="X" l="ENG"><s0>III-V compound</s0>
<s5>09</s5>
</fC07>
<fC07 i1="01" i2="X" l="SPA"><s0>Compuesto III-V</s0>
<s5>09</s5>
</fC07>
<fN21><s1>346</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
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