Hot-electron drift velocity and hot-phonon decay in AlInN/AlN/GaN
Identifieur interne : 002D12 ( Main/Repository ); précédent : 002D11; suivant : 002D13Hot-electron drift velocity and hot-phonon decay in AlInN/AlN/GaN
Auteurs : RBID : Pascal:11-0238920Descripteurs français
- Pascal (Inist)
- Electron chaud, Mobilité dérive, Vitesse dérive, Courant impulsionnel, Caractéristique courant tension, Mobilité électron, Champ uniforme, Effet champ électrique, Champ intense, Aluminium Indium Nitrure Mixte, Nitrure d'aluminium, Nitrure de gallium, Gaz électron 2 dimensions, Hétérostructure, Semiconducteur.
English descriptors
- KwdEn :
Abstract
A nanosecond-pulsed current-voltage technique was applied to study hot-electron transport along the two-dimensional electron gas channel confined at a nominally undoped AlInN/AlN/GaN heterointerface. Hot-electron drift velocity was deduced under the assumptions of uniform longitudinal electric field and field-independent electron sheet density. At a fixed electric field strength, a resonance-type non-monotonous dependence of the velocity on the electron density was found in the investigated range from I to 1.6 × 1013 cm-2. When the electric field increased from 20 kV/cm to 80 kV/cm, the peak velocity increased from ˜1.1 to 2.3 × 107 cm/s, and the position of the resonance shifted from ˜1.1 × 1013 cm-2 to ˜1.2 × 1013 cm-2, respectively. The resonance position correlates with that for the fastest decay of hot phonons known from independent experiment.
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<author><name sortKey="Ardaravicius, L" uniqKey="Ardaravicius L">L. Ardaravicius</name>
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<term>Aluminium nitride</term>
<term>Drift mobility</term>
<term>Drift velocity</term>
<term>Electric field effects</term>
<term>Electron mobility</term>
<term>Gallium nitride</term>
<term>Heterostructures</term>
<term>High field</term>
<term>Hot electrons</term>
<term>IV characteristic</term>
<term>Pulse current</term>
<term>Semiconductor materials</term>
<term>Two-dimensional electron gas</term>
<term>Uniform field</term>
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<term>Mobilité dérive</term>
<term>Vitesse dérive</term>
<term>Courant impulsionnel</term>
<term>Caractéristique courant tension</term>
<term>Mobilité électron</term>
<term>Champ uniforme</term>
<term>Effet champ électrique</term>
<term>Champ intense</term>
<term>Aluminium Indium Nitrure Mixte</term>
<term>Nitrure d'aluminium</term>
<term>Nitrure de gallium</term>
<term>Gaz électron 2 dimensions</term>
<term>Hétérostructure</term>
<term>Semiconducteur</term>
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<front><div type="abstract" xml:lang="en">A nanosecond-pulsed current-voltage technique was applied to study hot-electron transport along the two-dimensional electron gas channel confined at a nominally undoped AlInN/AlN/GaN heterointerface. Hot-electron drift velocity was deduced under the assumptions of uniform longitudinal electric field and field-independent electron sheet density. At a fixed electric field strength, a resonance-type non-monotonous dependence of the velocity on the electron density was found in the investigated range from I to 1.6 × 10<sup>13</sup>
cm<sup>-2</sup>
. When the electric field increased from 20 kV/cm to 80 kV/cm, the peak velocity increased from ˜1.1 to 2.3 × 10<sup>7</sup>
cm/s, and the position of the resonance shifted from ˜1.1 × 10<sup>13</sup>
cm<sup>-2</sup>
to ˜1.2 × 10<sup>13</sup>
cm<sup>-2</sup>
, respectively. The resonance position correlates with that for the fastest decay of hot phonons known from independent experiment.</div>
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<fC01 i1="01" l="ENG"><s0>A nanosecond-pulsed current-voltage technique was applied to study hot-electron transport along the two-dimensional electron gas channel confined at a nominally undoped AlInN/AlN/GaN heterointerface. Hot-electron drift velocity was deduced under the assumptions of uniform longitudinal electric field and field-independent electron sheet density. At a fixed electric field strength, a resonance-type non-monotonous dependence of the velocity on the electron density was found in the investigated range from I to 1.6 × 10<sup>13</sup>
cm<sup>-2</sup>
. When the electric field increased from 20 kV/cm to 80 kV/cm, the peak velocity increased from ˜1.1 to 2.3 × 10<sup>7</sup>
cm/s, and the position of the resonance shifted from ˜1.1 × 10<sup>13</sup>
cm<sup>-2</sup>
to ˜1.2 × 10<sup>13</sup>
cm<sup>-2</sup>
, respectively. The resonance position correlates with that for the fastest decay of hot phonons known from independent experiment.</s0>
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<s5>03</s5>
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<s5>03</s5>
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<s5>04</s5>
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<s5>04</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE"><s0>Courant impulsionnel</s0>
<s5>06</s5>
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<fC03 i1="04" i2="X" l="ENG"><s0>Pulse current</s0>
<s5>06</s5>
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<s5>06</s5>
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<s5>07</s5>
</fC03>
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<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Mobilité électron</s0>
<s5>08</s5>
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<s5>08</s5>
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<s2>NA</s2>
<s5>13</s5>
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<fC03 i1="10" i2="X" l="ENG"><s0>Aluminium Indium Nitrides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
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<s2>NA</s2>
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<s5>17</s5>
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<s5>17</s5>
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<s5>18</s5>
</fC03>
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<s5>18</s5>
</fC03>
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