Electrical properties of Au/polyvinylidene fluoride/n-InP Schottky diode with polymer interlayer
Identifieur interne : 000142 ( Main/Repository ); précédent : 000141; suivant : 000143Electrical properties of Au/polyvinylidene fluoride/n-InP Schottky diode with polymer interlayer
Auteurs : RBID : Pascal:14-0095744Descripteurs français
- Pascal (Inist)
- Propriété électrique, Vinylidène fluorure polymère, Semiconducteur III-V, Composé III-V, Diode barrière Schottky, Polymère, Couche intermédiaire, Effet redresseur, Caractéristique courant tension, Caractéristique capacité tension, Mesure tension électrique, Hauteur barrière, Couche mince, Charge espace, Résultat expérimental, Etat interface, Densité état, Courant fuite, Capacité électrique, Or, Phosphure d'indium, InP, Substrat polymère, 7350, 8105E, 8530K, 8530H.
- Wicri :
English descriptors
- KwdEn :
- Barrier height, CV characteristic, Capacitance, Density of states, Electrical properties, Experimental result, Gold, III-V compound, III-V semiconductors, IV characteristic, Indium phosphide, Interface states, Interlayers, Leakage currents, Polymers, Rectification, Schottky barrier diodes, Space charge, Thin films, Vinylidene fluoride polymer, Voltage measurement.
Abstract
The effect of polyvinylidene fluoride (PVDF) polymer interlayer on the rectifying junction parameters of Au/n-InP Schottky diode has been investigated using current-voltage (I-V) and capacitance-voltage (C-V) measurements at room temperature. The calculated barrier heights (BHs) are 0.57 eV (I-V), 0.72 eV (C-V) and 0.73 eV (I-V), 0.88 eV (C-V) for the Au/n-InP and Au/PVDF/n-InP Schottky diodes, respectively. Results showed that the BH of the Au/PVDF/n-InP Schottky diode is higher than that of the Au/n-InP Schottky diode, and that the PVDF film increases the effective BH by influencing the space charge region of the n-type InP. The values of the barrier height, ideality factors and series resistance estimated by I-V, Cheung's and Norde methods are compared. Experimental results showed that the interface state density of the Au/PVDF/n-InP Schottky diode is lower than that of the Au/n-InPSchottky diode. Further, the reverse leakage current conduction mechanism is investigated. Schottky emission mechanism is found to dominate the reverse leakage current in the Au/n-InP Schottky diode. However, for the Au/PVDF/n-InP Schottky diode, the Schottky conduction mechanism is found to be dominant in the higher bias region, whereas the Poole-Frenkel conduction is found to be dominant in the lower bias region. Apart from that, the discrepancy between BHs determined from I-V and C-V techniques is explained. Besides, the capacitance-frequency (C-f) and conductance-frequency (G-f) characteristics of the Au/PVDF/n-InP Schottky diode are discussed.
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<author><name sortKey="Rajagopal Reddy, V" uniqKey="Rajagopal Reddy V">V. Rajagopal Reddy</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physics, Sri Venkateswara University</s1>
<s2>Tirupati 517 502</s2>
<s3>IND</s3>
<sZ>1 aut.</sZ>
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<country>Inde</country>
<wicri:noRegion>Tirupati 517 502</wicri:noRegion>
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<publicationStmt><idno type="inist">14-0095744</idno>
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<title level="j" type="abbreviated">Thin solid films</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Barrier height</term>
<term>CV characteristic</term>
<term>Capacitance</term>
<term>Density of states</term>
<term>Electrical properties</term>
<term>Experimental result</term>
<term>Gold</term>
<term>III-V compound</term>
<term>III-V semiconductors</term>
<term>IV characteristic</term>
<term>Indium phosphide</term>
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<term>Interlayers</term>
<term>Leakage currents</term>
<term>Polymers</term>
<term>Rectification</term>
<term>Schottky barrier diodes</term>
<term>Space charge</term>
<term>Thin films</term>
<term>Vinylidene fluoride polymer</term>
<term>Voltage measurement</term>
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<keywords scheme="Pascal" xml:lang="fr"><term>Propriété électrique</term>
<term>Vinylidène fluorure polymère</term>
<term>Semiconducteur III-V</term>
<term>Composé III-V</term>
<term>Diode barrière Schottky</term>
<term>Polymère</term>
<term>Couche intermédiaire</term>
<term>Effet redresseur</term>
<term>Caractéristique courant tension</term>
<term>Caractéristique capacité tension</term>
<term>Mesure tension électrique</term>
<term>Hauteur barrière</term>
<term>Couche mince</term>
<term>Charge espace</term>
<term>Résultat expérimental</term>
<term>Etat interface</term>
<term>Densité état</term>
<term>Courant fuite</term>
<term>Capacité électrique</term>
<term>Or</term>
<term>Phosphure d'indium</term>
<term>InP</term>
<term>Substrat polymère</term>
<term>7350</term>
<term>8105E</term>
<term>8530K</term>
<term>8530H</term>
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<keywords scheme="Wicri" type="concept" xml:lang="fr"><term>Polymère</term>
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<front><div type="abstract" xml:lang="en">The effect of polyvinylidene fluoride (PVDF) polymer interlayer on the rectifying junction parameters of Au/n-InP Schottky diode has been investigated using current-voltage (I-V) and capacitance-voltage (C-V) measurements at room temperature. The calculated barrier heights (BHs) are 0.57 eV (I-V), 0.72 eV (C-V) and 0.73 eV (I-V), 0.88 eV (C-V) for the Au/n-InP and Au/PVDF/n-InP Schottky diodes, respectively. Results showed that the BH of the Au/PVDF/n-InP Schottky diode is higher than that of the Au/n-InP Schottky diode, and that the PVDF film increases the effective BH by influencing the space charge region of the n-type InP. The values of the barrier height, ideality factors and series resistance estimated by I-V, Cheung's and Norde methods are compared. Experimental results showed that the interface state density of the Au/PVDF/n-InP Schottky diode is lower than that of the Au/n-InPSchottky diode. Further, the reverse leakage current conduction mechanism is investigated. Schottky emission mechanism is found to dominate the reverse leakage current in the Au/n-InP Schottky diode. However, for the Au/PVDF/n-InP Schottky diode, the Schottky conduction mechanism is found to be dominant in the higher bias region, whereas the Poole-Frenkel conduction is found to be dominant in the lower bias region. Apart from that, the discrepancy between BHs determined from I-V and C-V techniques is explained. Besides, the capacitance-frequency (C-f) and conductance-frequency (G-f) characteristics of the Au/PVDF/n-InP Schottky diode are discussed.</div>
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<fA11 i1="01" i2="1"><s1>RAJAGOPAL REDDY (V.)</s1>
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<fA14 i1="01"><s1>Department of Physics, Sri Venkateswara University</s1>
<s2>Tirupati 517 502</s2>
<s3>IND</s3>
<sZ>1 aut.</sZ>
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<fC01 i1="01" l="ENG"><s0>The effect of polyvinylidene fluoride (PVDF) polymer interlayer on the rectifying junction parameters of Au/n-InP Schottky diode has been investigated using current-voltage (I-V) and capacitance-voltage (C-V) measurements at room temperature. The calculated barrier heights (BHs) are 0.57 eV (I-V), 0.72 eV (C-V) and 0.73 eV (I-V), 0.88 eV (C-V) for the Au/n-InP and Au/PVDF/n-InP Schottky diodes, respectively. Results showed that the BH of the Au/PVDF/n-InP Schottky diode is higher than that of the Au/n-InP Schottky diode, and that the PVDF film increases the effective BH by influencing the space charge region of the n-type InP. The values of the barrier height, ideality factors and series resistance estimated by I-V, Cheung's and Norde methods are compared. Experimental results showed that the interface state density of the Au/PVDF/n-InP Schottky diode is lower than that of the Au/n-InPSchottky diode. Further, the reverse leakage current conduction mechanism is investigated. Schottky emission mechanism is found to dominate the reverse leakage current in the Au/n-InP Schottky diode. However, for the Au/PVDF/n-InP Schottky diode, the Schottky conduction mechanism is found to be dominant in the higher bias region, whereas the Poole-Frenkel conduction is found to be dominant in the lower bias region. Apart from that, the discrepancy between BHs determined from I-V and C-V techniques is explained. Besides, the capacitance-frequency (C-f) and conductance-frequency (G-f) characteristics of the Au/PVDF/n-InP Schottky diode are discussed.</s0>
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<s2>NK</s2>
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<s5>14</s5>
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<s5>14</s5>
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<s5>29</s5>
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<fC03 i1="15" i2="X" l="ENG"><s0>Experimental result</s0>
<s5>29</s5>
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<s5>30</s5>
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<s5>30</s5>
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<s5>31</s5>
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<fC03 i1="17" i2="X" l="ENG"><s0>Density of states</s0>
<s5>31</s5>
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<s5>31</s5>
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<s5>32</s5>
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<s5>33</s5>
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<s5>33</s5>
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<s2>NC</s2>
<s5>34</s5>
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<s2>NC</s2>
<s5>34</s5>
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<s5>35</s5>
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<s5>46</s5>
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<s4>INC</s4>
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<s4>INC</s4>
<s5>72</s5>
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<fC03 i1="26" i2="3" l="FRE"><s0>8530K</s0>
<s4>INC</s4>
<s5>73</s5>
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<s4>INC</s4>
<s5>74</s5>
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