IndiumV3, Chine, Analysis, bibRecord, 000A58

Quantum dot multi-wavelength comb lasers with Si ring resonator

Identifieur interne : 000A58 ( Chine/Analysis ); précédent : 000A57; suivant : 000A59

Quantum dot multi-wavelength comb lasers with Si ring resonator

Auteurs : RBID : Pascal:11-0161100

Descripteurs français

Pascal (Inist)
- Laser semiconducteur, Résonateur anneau, Laser point quantique, Point quantique, Composé binaire, Indium Arséniure, Composé quaternaire, Gallium Arséniure, Indium Phosphure, Gallium Phosphure, Silicium, InAs, InGaAsP, Substrat InP, As In, As Ga In P, Longueur cavité, 0130C, 42, 4255P, Photonique.

English descriptors

KwdEn :
- Binary compounds, Gallium Arsenides, Gallium Phosphides, Indium Arsenides, Indium Phosphides, Photonics, Quantum dot lasers, Quantum dots, Quaternary compounds, Ring resonator, Semiconductor lasers, Silicon.

Abstract

The gain media of the quantum dot lasers consist of InAs QDs in an InGaAsP matrix on an InP substrate. The quantum dot lasers have different free spacing ranges (FSRs) corresponding to Fabry-Pérot (F-P) cavity lengths. A silicon ring resonator and a QD laser have been combined to form comb laser .The output characteristics of the combined comb laser were investigated. The measured FSR was about 2.8nm and the extinction ratio was about 10(dB) when the FSR of the QD laser was about 0.4nm and the FSR of the ring resonator was about 0.47nm. The experimental results show that the ring resonator had a strong control on the FSR and extinction ratio of the comb laser.

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Pascal:11-0161100

Le document en format XML

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<author><name sortKey="Lu, Z G" uniqKey="Lu Z">Z. G. Lu</name>
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<author><name sortKey="Janz, S" uniqKey="Janz S">S. Janz</name>
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<date when="2010">2010</date>
<idno type="stanalyst">PASCAL 11-0161100 INIST</idno>
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<seriesStmt><idno type="ISSN">0277-786X</idno>
<title level="j" type="abbreviated">Proc. SPIE Int. Soc. Opt. Eng.</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Binary compounds</term>
<term>Gallium Arsenides</term>
<term>Gallium Phosphides</term>
<term>Indium Arsenides</term>
<term>Indium Phosphides</term>
<term>Photonics</term>
<term>Quantum dot lasers</term>
<term>Quantum dots</term>
<term>Quaternary compounds</term>
<term>Ring resonator</term>
<term>Semiconductor lasers</term>
<term>Silicon</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Laser semiconducteur</term>
<term>Résonateur anneau</term>
<term>Laser point quantique</term>
<term>Point quantique</term>
<term>Composé binaire</term>
<term>Indium Arséniure</term>
<term>Composé quaternaire</term>
<term>Gallium Arséniure</term>
<term>Indium Phosphure</term>
<term>Gallium Phosphure</term>
<term>Silicium</term>
<term>InAs</term>
<term>InGaAsP</term>
<term>Substrat InP</term>
<term>As In</term>
<term>As Ga In P</term>
<term>Longueur cavité</term>
<term>0130C</term>
<term>42</term>
<term>4255P</term>
<term>Photonique</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">The gain media of the quantum dot lasers consist of InAs QDs in an InGaAsP matrix on an InP substrate. The quantum dot lasers have different free spacing ranges (FSRs) corresponding to Fabry-Pérot (F-P) cavity lengths. A silicon ring resonator and a QD laser have been combined to form comb laser .The output characteristics of the combined comb laser were investigated. The measured FSR was about 2.8nm and the extinction ratio was about 10(dB) when the FSR of the QD laser was about 0.4nm and the FSR of the ring resonator was about 0.47nm. The experimental results show that the ring resonator had a strong control on the FSR and extinction ratio of the comb laser.</div>
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<fA08 i1="01" i2="1" l="ENG"><s1>Quantum dot multi-wavelength comb lasers with Si ring resonator</s1>
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<fA09 i1="01" i2="1" l="ENG"><s1>Photonics North 2010 : 1-3 June 2010, Niagara Falls, Canada</s1>
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<fA11 i1="01" i2="1"><s1>LI (W. Y.)</s1>
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<fA11 i1="02" i2="1"><s1>LU (Z. G.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>XU (D. X.)</s1>
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<fA11 i1="04" i2="1"><s1>LIU (J. R.)</s1>
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<fA11 i1="07" i2="1"><s1>POITRAS (D.)</s1>
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<fA11 i1="08" i2="1"><s1>MA (R.)</s1>
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<fA11 i1="09" i2="1"><s1>LAPOINTE (J.)</s1>
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<fA11 i1="10" i2="1"><s1>VACHON (M.)</s1>
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<fA12 i1="01" i2="1"><s1>SCHRIEMER (Henry P.)</s1>
<s9>ed.</s9>
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<fA12 i1="02" i2="1"><s1>KLEIMAN (Rafael N.)</s1>
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<fA14 i1="01"><s1>Ins. for Microstructural Sciences, National Research Council</s1>
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<fA14 i1="02"><s1>National University of Defense Technology</s1>
<s2>Changsha, Hunan</s2>
<s3>CHN</s3>
<sZ>1 aut.</sZ>
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<fA18 i1="01" i2="1"><s1>Ontario Photonics Industry Network</s1>
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<s9>org-cong.</s9>
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<fA60><s1>P</s1>
<s2>C</s2>
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</fA61>
<fA64 i1="01" i2="1"><s0>Proceedings of SPIE, the International Society for Optical Engineering</s0>
</fA64>
<fA66 i1="01"><s0>USA</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>The gain media of the quantum dot lasers consist of InAs QDs in an InGaAsP matrix on an InP substrate. The quantum dot lasers have different free spacing ranges (FSRs) corresponding to Fabry-Pérot (F-P) cavity lengths. A silicon ring resonator and a QD laser have been combined to form comb laser .The output characteristics of the combined comb laser were investigated. The measured FSR was about 2.8nm and the extinction ratio was about 10(dB) when the FSR of the QD laser was about 0.4nm and the FSR of the ring resonator was about 0.47nm. The experimental results show that the ring resonator had a strong control on the FSR and extinction ratio of the comb laser.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B00A30C</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B40B55P</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Laser semiconducteur</s0>
<s5>09</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Semiconductor lasers</s0>
<s5>09</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Résonateur anneau</s0>
<s5>11</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG"><s0>Ring resonator</s0>
<s5>11</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA"><s0>Resonador anillo</s0>
<s5>11</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Laser point quantique</s0>
<s5>12</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Quantum dot lasers</s0>
<s5>12</s5>
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<fC03 i1="04" i2="3" l="FRE"><s0>Point quantique</s0>
<s5>47</s5>
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<fC03 i1="04" i2="3" l="ENG"><s0>Quantum dots</s0>
<s5>47</s5>
</fC03>
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<s5>50</s5>
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<s5>50</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Indium Arséniure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>51</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Indium Arsenides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>51</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Composé quaternaire</s0>
<s5>52</s5>
</fC03>
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<s5>52</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Gallium Arséniure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>53</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Gallium Arsenides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>53</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Indium Phosphure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>54</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Indium Phosphides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>54</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Gallium Phosphure</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>55</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Gallium Phosphides</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>55</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Silicium</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Silicon</s0>
<s2>NC</s2>
<s5>61</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>InAs</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>InGaAsP</s0>
<s4>INC</s4>
<s5>72</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Substrat InP</s0>
<s4>INC</s4>
<s5>73</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>As In</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>As Ga In P</s0>
<s4>INC</s4>
<s5>76</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Longueur cavité</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>0130C</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>42</s0>
<s4>INC</s4>
<s5>85</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>4255P</s0>
<s4>INC</s4>
<s5>91</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>Photonique</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="21" i2="3" l="ENG"><s0>Photonics</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fN21><s1>101</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
</pA>
<pR><fA30 i1="01" i2="1" l="ENG"><s1>Photonics North 2010</s1>
<s3>Niagara Falls CAN</s3>
<s4>2010</s4>
</fA30>
</pR>
</standard>
</inist>
</record>

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   |texte=   Quantum dot multi-wavelength comb lasers with Si ring resonator
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Quantum dot multi-wavelength comb lasers with Si ring resonator

Quantum dot multi-wavelength comb lasers with Si ring resonator

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