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Optical and Magnetic Properties of Ten-Period InGaMnAs/GaAs Quantum Wells

Identifieur interne : 000802 ( Main/Repository ); précédent : 000801; suivant : 000803

Optical and Magnetic Properties of Ten-Period InGaMnAs/GaAs Quantum Wells

Auteurs : RBID : Pascal:14-0008358

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English descriptors

Abstract

Ten layers of InGaMnAs/GaAs multiquantum wells (MQWs) structure were grown on high resistivity (100) p-type GaAs substrates by molecular beam epitaxy (MBE). A presence of the ferromagnetic structure was confirmed in the InGaMnAs/GaAs MQWs structure, and have ferromagnetic ordering with a Curie temperature, TC = 50 K. It is likely that the ferromagnetic exchange coupling of the sample with TC = 50 K is hole-mediated resulting in Mn substituting In or Ga sites. PL emission spectra of the InGaMnAs MQWs sample grown at a temperature of 170 °C show that an activation energy of the Mn ion on the first quantum confinement level in InGaAs QW is 32 meV and impurity Mn is partly ionized. The fact that the activation energy of 32 meV of Mn ion in the QW is lower than an activation energy of 110 meV for a substitutional Mn impurity in GaAs, indicating an impurity band existing in the bandgap due to substitutional Mn ions.

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<term>Exchange interactions</term>
<term>Ferromagnetic materials</term>
<term>Ferromagnetism</term>
<term>Gallium</term>
<term>Gallium Arsenides</term>
<term>Gallium arsenides</term>
<term>III-V semiconductors</term>
<term>Indium Arsenides</term>
<term>Indium arsenides</term>
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<term>Magnetic properties</term>
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<term>Indium Arséniure</term>
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<term>Puits quantique</term>
<term>Matériau ferromagnétique</term>
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<term>Luminescence</term>
<term>Energie activation</term>
<term>Confinement quantique</term>
<term>Arséniure d'indium</term>
<term>Impureté substitutionnelle</term>
<term>As Ga</term>
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<div type="abstract" xml:lang="en">Ten layers of InGaMnAs/GaAs multiquantum wells (MQWs) structure were grown on high resistivity (100) p-type GaAs substrates by molecular beam epitaxy (MBE). A presence of the ferromagnetic structure was confirmed in the InGaMnAs/GaAs MQWs structure, and have ferromagnetic ordering with a Curie temperature, T
<sub>C</sub>
= 50 K. It is likely that the ferromagnetic exchange coupling of the sample with T
<sub>C</sub>
= 50 K is hole-mediated resulting in Mn substituting In or Ga sites. PL emission spectra of the InGaMnAs MQWs sample grown at a temperature of 170 °C show that an activation energy of the Mn ion on the first quantum confinement level in InGaAs QW is 32 meV and impurity Mn is partly ionized. The fact that the activation energy of 32 meV of Mn ion in the QW is lower than an activation energy of 110 meV for a substitutional Mn impurity in GaAs, indicating an impurity band existing in the bandgap due to substitutional Mn ions.</div>
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<s0>Ten layers of InGaMnAs/GaAs multiquantum wells (MQWs) structure were grown on high resistivity (100) p-type GaAs substrates by molecular beam epitaxy (MBE). A presence of the ferromagnetic structure was confirmed in the InGaMnAs/GaAs MQWs structure, and have ferromagnetic ordering with a Curie temperature, T
<sub>C</sub>
= 50 K. It is likely that the ferromagnetic exchange coupling of the sample with T
<sub>C</sub>
= 50 K is hole-mediated resulting in Mn substituting In or Ga sites. PL emission spectra of the InGaMnAs MQWs sample grown at a temperature of 170 °C show that an activation energy of the Mn ion on the first quantum confinement level in InGaAs QW is 32 meV and impurity Mn is partly ionized. The fact that the activation energy of 32 meV of Mn ion in the QW is lower than an activation energy of 110 meV for a substitutional Mn impurity in GaAs, indicating an impurity band existing in the bandgap due to substitutional Mn ions.</s0>
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<s5>43</s5>
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<s5>44</s5>
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<s5>44</s5>
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<s5>52</s5>
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<s0>Gallium Arsenides</s0>
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<s2>NA</s2>
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<fC03 i1="10" i2="3" l="FRE">
<s0>Indium Arséniure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>53</s5>
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<fC03 i1="10" i2="3" l="ENG">
<s0>Indium Arsenides</s0>
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<s2>NA</s2>
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<s5>64</s5>
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<s0>Gallium</s0>
<s2>NC</s2>
<s5>64</s5>
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<s5>65</s5>
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<s0>Luminescence</s0>
<s5>65</s5>
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<s0>Energie activation</s0>
<s5>66</s5>
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<s5>66</s5>
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<s5>67</s5>
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<s0>Quantum confinement</s0>
<s5>67</s5>
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<fC03 i1="17" i2="X" l="SPA">
<s0>Confinamiento cuántico</s0>
<s5>67</s5>
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<s0>Arséniure d'indium</s0>
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<s5>68</s5>
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<s5>68</s5>
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<s0>Impureté substitutionnelle</s0>
<s5>69</s5>
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<s0>Substitutional impurities</s0>
<s5>69</s5>
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<s0>Impureza substitucional</s0>
<s5>69</s5>
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<s0>As Ga</s0>
<s4>INC</s4>
<s5>75</s5>
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<fC03 i1="21" i2="3" l="FRE">
<s0>As Ga In</s0>
<s4>INC</s4>
<s5>76</s5>
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<fC03 i1="22" i2="3" l="FRE">
<s0>GaAs</s0>
<s4>INC</s4>
<s5>83</s5>
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<fC03 i1="23" i2="3" l="FRE">
<s0>Substrat GaAs</s0>
<s4>INC</s4>
<s5>84</s5>
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<fC03 i1="24" i2="3" l="FRE">
<s0>7530E</s0>
<s4>INC</s4>
<s5>85</s5>
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<fC03 i1="25" i2="3" l="FRE">
<s0>InGaAs</s0>
<s4>INC</s4>
<s5>86</s5>
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<fN21>
<s1>006</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
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