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Characterisation of the LPE grown InGaAsP/InP hetero-structures : IR-LED at 1.66 μm used for the remote monitoring of methane gas

Identifieur interne : 001131 ( Russie/Analysis ); précédent : 001130; suivant : 001132

Characterisation of the LPE grown InGaAsP/InP hetero-structures : IR-LED at 1.66 μm used for the remote monitoring of methane gas

Auteurs : RBID : Pascal:97-0328744

Descripteurs français

English descriptors

Abstract

Combined TEM, HREM, ED, SIMS, X-ray and electroluminescence studies were used to characterise in detail a highly effective IR-LED emitting at the wavelength 1.66 μm and based on buried heterostructure In0.88Ga0.12As0.26P0.74/In0.72Ga0.28As0.62P0.38/In0.53Ga0.47As/InP grown by liquid-phase epitaxy. The InGaAsP epilayers were found to be well lattice-matched, dislocation free and of good structural quality. A tentative explanation is presented for the spinodal decomposition observed in InGaAsP alloys. A new type of selective methane gas sensor has been developed and fabricated on the basis of the IR-light emitting diode mentioned above. It is shown that the proposed type of sensor can be used for the quantitative remote control of methane gas concentration (0.2-100%) via a fibre glass line up to the distance of 2 x 1 km.

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Pascal:97-0328744

Le document en format XML

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<name sortKey="Volkov, V V" uniqKey="Volkov V">V. V. Volkov</name>
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<s1>N.S. Kurnakov Institute of General and Inorganic Chemistry, RAS, Leninsky Prospect 31, GSP-1</s1>
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<name sortKey="Sokolovsky, A A" uniqKey="Sokolovsky A">A. A. Sokolovsky</name>
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<sZ>8 aut.</sZ>
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<date when="1997">1997</date>
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<term>Absorbance</term>
<term>Crystal growth</term>
<term>Gallium Arsenides</term>
<term>Gallium Phosphides</term>
<term>Gas detector</term>
<term>Heterojunction</term>
<term>Indium Arsenides</term>
<term>Indium Phosphides</term>
<term>Infrared detection</term>
<term>Light emitting diode</term>
<term>Methane</term>
<term>Partial pressure</term>
<term>Phase separation</term>
<term>Pressure effect</term>
<term>Remote sensing</term>
<term>Spinodal curve</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Diode électroluminescente</term>
<term>Détection IR</term>
<term>Détecteur de gaz</term>
<term>Télédétection</term>
<term>Méthane</term>
<term>Hétérojonction</term>
<term>Croissance cristalline</term>
<term>Indium Phosphure</term>
<term>Gallium Arséniure</term>
<term>Indium Arséniure</term>
<term>Gallium Phosphure</term>
<term>Séparation phase</term>
<term>Absorbance</term>
<term>Effet pression</term>
<term>Pression partielle</term>
<term>Courbe spinodale</term>
<term>InGaAsP</term>
<term>InP</term>
<term>As Ga In P</term>
<term>In P</term>
</keywords>
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<term>Télédétection</term>
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<div type="abstract" xml:lang="en">Combined TEM, HREM, ED, SIMS, X-ray and electroluminescence studies were used to characterise in detail a highly effective IR-LED emitting at the wavelength 1.66 μm and based on buried heterostructure In
<sub>0.88</sub>
Ga
<sub>0.12</sub>
As
<sub>0.26</sub>
P
<sub>0.74</sub>
/In
<sub>0.72</sub>
Ga
<sub>0.28</sub>
As
<sub>0.62</sub>
P
<sub>0.38</sub>
/In
<sub>0.53</sub>
Ga
<sub>0.47</sub>
As/InP grown by liquid-phase epitaxy. The InGaAsP epilayers were found to be well lattice-matched, dislocation free and of good structural quality. A tentative explanation is presented for the spinodal decomposition observed in InGaAsP alloys. A new type of selective methane gas sensor has been developed and fabricated on the basis of the IR-light emitting diode mentioned above. It is shown that the proposed type of sensor can be used for the quantitative remote control of methane gas concentration (0.2-100%) via a fibre glass line up to the distance of 2 x 1 km.</div>
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<s0>27 ref.</s0>
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<s1>P</s1>
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<s0>NLD</s0>
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<fC01 i1="01" l="ENG">
<s0>Combined TEM, HREM, ED, SIMS, X-ray and electroluminescence studies were used to characterise in detail a highly effective IR-LED emitting at the wavelength 1.66 μm and based on buried heterostructure In
<sub>0.88</sub>
Ga
<sub>0.12</sub>
As
<sub>0.26</sub>
P
<sub>0.74</sub>
/In
<sub>0.72</sub>
Ga
<sub>0.28</sub>
As
<sub>0.62</sub>
P
<sub>0.38</sub>
/In
<sub>0.53</sub>
Ga
<sub>0.47</sub>
As/InP grown by liquid-phase epitaxy. The InGaAsP epilayers were found to be well lattice-matched, dislocation free and of good structural quality. A tentative explanation is presented for the spinodal decomposition observed in InGaAsP alloys. A new type of selective methane gas sensor has been developed and fabricated on the basis of the IR-light emitting diode mentioned above. It is shown that the proposed type of sensor can be used for the quantitative remote control of methane gas concentration (0.2-100%) via a fibre glass line up to the distance of 2 x 1 km.</s0>
</fC01>
<fC02 i1="01" i2="X">
<s0>001D03F15</s0>
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<fC02 i1="02" i2="X">
<s0>001C04A</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE">
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<s5>50</s5>
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<s5>51</s5>
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<s5>51</s5>
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<s5>52</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG">
<s0>Gas detector</s0>
<s5>52</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA">
<s0>Detector de gas</s0>
<s5>52</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Télédétection</s0>
<s5>53</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Remote sensing</s0>
<s5>53</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Teledetección</s0>
<s5>53</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE">
<s0>Méthane</s0>
<s2>NK</s2>
<s2>FX</s2>
<s5>54</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG">
<s0>Methane</s0>
<s2>NK</s2>
<s2>FX</s2>
<s5>54</s5>
</fC03>
<fC03 i1="05" i2="X" l="GER">
<s0>Methan</s0>
<s2>NK</s2>
<s2>FX</s2>
<s5>54</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA">
<s0>Metano</s0>
<s2>NK</s2>
<s2>FX</s2>
<s5>54</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Hétérojonction</s0>
<s5>55</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Heterojunction</s0>
<s5>55</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Heterounión</s0>
<s5>55</s5>
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<fC03 i1="07" i2="X" l="FRE">
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<s5>56</s5>
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<s5>56</s5>
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<fC03 i1="07" i2="X" l="GER">
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<s5>56</s5>
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<s0>Crecimiento cristalino</s0>
<s5>56</s5>
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<fC03 i1="08" i2="X" l="FRE">
<s0>Indium Phosphure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>57</s5>
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<fC03 i1="08" i2="X" l="ENG">
<s0>Indium Phosphides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>57</s5>
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<fC03 i1="08" i2="X" l="SPA">
<s0>Indio Fosfuro</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>57</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Gallium Arséniure</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>58</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Gallium Arsenides</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>58</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Galio Arseniuro</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>58</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Indium Arséniure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>59</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>Indium Arsenides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>59</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Indio Arseniuro</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>59</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE">
<s0>Gallium Phosphure</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>60</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG">
<s0>Gallium Phosphides</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>60</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA">
<s0>Galio Fosfuro</s0>
<s2>NC</s2>
<s2>FX</s2>
<s2>NA</s2>
<s5>60</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE">
<s0>Séparation phase</s0>
<s5>61</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG">
<s0>Phase separation</s0>
<s5>61</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA">
<s0>Separación fase</s0>
<s5>61</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Absorbance</s0>
<s5>62</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>Absorbance</s0>
<s5>62</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA">
<s0>Absorbancia</s0>
<s5>62</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE">
<s0>Effet pression</s0>
<s5>63</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG">
<s0>Pressure effect</s0>
<s5>63</s5>
</fC03>
<fC03 i1="14" i2="X" l="GER">
<s0>Druckeinfluss</s0>
<s5>63</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA">
<s0>Efecto presión</s0>
<s5>63</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE">
<s0>Pression partielle</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG">
<s0>Partial pressure</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="X" l="GER">
<s0>Partialdruck</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA">
<s0>Presión parcial</s0>
<s5>64</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE">
<s0>Courbe spinodale</s0>
<s5>65</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG">
<s0>Spinodal curve</s0>
<s5>65</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA">
<s0>Curva spinodal</s0>
<s5>65</s5>
</fC03>
<fC03 i1="17" i2="X" l="FRE">
<s0>InGaAsP</s0>
<s4>INC</s4>
<s5>72</s5>
</fC03>
<fC03 i1="18" i2="X" l="FRE">
<s0>InP</s0>
<s4>INC</s4>
<s5>73</s5>
</fC03>
<fC03 i1="19" i2="X" l="FRE">
<s0>As Ga In P</s0>
<s4>INC</s4>
<s5>74</s5>
</fC03>
<fC03 i1="20" i2="X" l="FRE">
<s0>In P</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03>
<fN21>
<s1>188</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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