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Influence of thermal treatment in N2 atmosphere on chemical, microstructural and optical properties of indium tin oxide and nitrogen doped indium tin oxide rf-sputtered thin films

Identifieur interne : 000A34 ( Main/Repository ); précédent : 000A33; suivant : 000A35

Influence of thermal treatment in N2 atmosphere on chemical, microstructural and optical properties of indium tin oxide and nitrogen doped indium tin oxide rf-sputtered thin films

Auteurs : RBID : Pascal:13-0310109

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Abstract

We report the influence of the normal thermal treatment (TT) and of rapid thermal annealing (RTA) on the microstructural, optical and electrical properties of indium tin oxide (ITO) and nitrogen doped indium tin oxide (ITO:N) thin films. The TT was carried out for 1 h at 400 °C and the RTA for 1 min up to 400 °C, both in N2 atmosphere. The ITO and ITO:N films were deposited by reactive sputtering in Argon, and respectively Nitrogen plasma, on Si with (100) and (111) orientation. The present study brings data about the microstructural and optical properties of ITO thin films with thicknesses around 300-400 nm. Atomic Force Microscopy analysis showed the formation of continuous and homogeneous films, fully covered by quasi-spherical shaped particles, with higher roughness values on Si(100) as compared to Si(111). Spectroscopic ellipsometry allowed the determination of film thickness, optical band gap as well as of the dispersion curves of n and k optical constants. X-ray diffraction analysis revealed the presence of diffraction peaks corresponding to the same nominal bulk composition of ITO, but with different intensities and preferential orientation depending on the substrate, atmosphere of deposition and type of thermal treatment.

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Pascal:13-0310109

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<div type="abstract" xml:lang="en">We report the influence of the normal thermal treatment (TT) and of rapid thermal annealing (RTA) on the microstructural, optical and electrical properties of indium tin oxide (ITO) and nitrogen doped indium tin oxide (ITO:N) thin films. The TT was carried out for 1 h at 400 °C and the RTA for 1 min up to 400 °C, both in N
<sub>2</sub>
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<fC03 i1="11" i2="3" l="FRE">
<s0>Recuit thermique rapide</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Rapid thermal annealing</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Propriété électrique</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Electrical properties</s0>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Pulvérisation réactive</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Reactive sputtering</s0>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Dépôt physique phase vapeur</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Physical vapor deposition</s0>
<s5>14</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE">
<s0>Epaisseur couche</s0>
<s5>29</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG">
<s0>Layer thickness</s0>
<s5>29</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA">
<s0>Espesor capa</s0>
<s5>29</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE">
<s0>Nanomatériau</s0>
<s5>30</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG">
<s0>Nanostructured materials</s0>
<s5>30</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE">
<s0>Microscopie force atomique</s0>
<s5>31</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG">
<s0>Atomic force microscopy</s0>
<s5>31</s5>
</fC03>
<fC03 i1="18" i2="X" l="FRE">
<s0>Particule sphérique</s0>
<s5>32</s5>
</fC03>
<fC03 i1="18" i2="X" l="ENG">
<s0>Spherical particle</s0>
<s5>32</s5>
</fC03>
<fC03 i1="18" i2="X" l="SPA">
<s0>Partícula esférica</s0>
<s5>32</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE">
<s0>Rugosité</s0>
<s5>33</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG">
<s0>Roughness</s0>
<s5>33</s5>
</fC03>
<fC03 i1="20" i2="X" l="FRE">
<s0>Ellipsométrie spectroscopique</s0>
<s5>34</s5>
</fC03>
<fC03 i1="20" i2="X" l="ENG">
<s0>Spectroscopic ellipsometry</s0>
<s5>34</s5>
</fC03>
<fC03 i1="20" i2="X" l="SPA">
<s0>Elipsometría espectroscópica</s0>
<s5>34</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE">
<s0>Bande interdite photonique</s0>
<s5>35</s5>
</fC03>
<fC03 i1="21" i2="3" l="ENG">
<s0>Photonic band gap</s0>
<s5>35</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE">
<s0>Dispersion</s0>
<s5>36</s5>
</fC03>
<fC03 i1="22" i2="3" l="ENG">
<s0>Dispersions</s0>
<s5>36</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE">
<s0>Constante optique</s0>
<s5>37</s5>
</fC03>
<fC03 i1="23" i2="3" l="ENG">
<s0>Optical constants</s0>
<s5>37</s5>
</fC03>
<fC03 i1="24" i2="3" l="FRE">
<s0>Analyse diffraction RX</s0>
<s5>38</s5>
</fC03>
<fC03 i1="24" i2="3" l="ENG">
<s0>X-ray diffraction analysis</s0>
<s5>38</s5>
</fC03>
<fC03 i1="25" i2="X" l="FRE">
<s0>Orientation préférentielle</s0>
<s5>39</s5>
</fC03>
<fC03 i1="25" i2="X" l="ENG">
<s0>Preferred orientation</s0>
<s5>39</s5>
</fC03>
<fC03 i1="25" i2="X" l="SPA">
<s0>Orientación preferencial</s0>
<s5>39</s5>
</fC03>
<fC03 i1="26" i2="X" l="FRE">
<s0>Pulvérisation haute fréquence</s0>
<s5>40</s5>
</fC03>
<fC03 i1="26" i2="X" l="ENG">
<s0>Radiofrequency sputtering</s0>
<s5>40</s5>
</fC03>
<fC03 i1="26" i2="X" l="SPA">
<s0>Pulverización alta frecuencia</s0>
<s5>40</s5>
</fC03>
<fC03 i1="27" i2="3" l="FRE">
<s0>Substrat silicium</s0>
<s4>INC</s4>
<s5>46</s5>
</fC03>
<fC03 i1="28" i2="3" l="FRE">
<s0>6855J</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fC03 i1="29" i2="3" l="FRE">
<s0>7866</s0>
<s4>INC</s4>
<s5>72</s5>
</fC03>
<fC03 i1="30" i2="3" l="FRE">
<s0>8115C</s0>
<s4>INC</s4>
<s5>73</s5>
</fC03>
<fC03 i1="31" i2="3" l="FRE">
<s0>7350</s0>
<s4>INC</s4>
<s5>74</s5>
</fC03>
<fN21>
<s1>294</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
<pR>
<fA30 i1="01" i2="1" l="ENG">
<s1>"Current Trends in Optical and X-Ray Metrology of Advanced Materials for Nanoscale Devices III", E-MRS Spring-Symposium W</s1>
<s3>Strasbourg FRA</s3>
<s4>2012-05-14</s4>
</fA30>
</pR>
</standard>
</inist>
</record>

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