Pressure and temperature dependence of gain in InGaAs/GaAs laser diode
Identifieur interne : 001655 ( Main/Repository ); précédent : 001654; suivant : 001656Pressure and temperature dependence of gain in InGaAs/GaAs laser diode
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Abstract
Wavelength dependent gain has been calculated for InGaAs/ GaAs quantum-well (QW) lasers as a function of hydrostatic pressure and temperature. The shift of the gain maximum for such laser is equal to -140 nm by increasing the pressure up to 20 kbar and -60 nm by cooling down from 300 to 100 K. The width of the gain curve (determining the possible tuning range with external grating) is significantly reduced at low temperatures and (to a lower extent) at high pressures. Our results indicate that pressure tuning is much more effective than temperature tuning when combined with tuning by external grating.
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<author><name sortKey="Bajda, Monika" uniqKey="Bajda M">Monika Bajda</name>
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<author><name sortKey="Bercha, Artem" uniqKey="Bercha A">Artem Bercha</name>
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<author><name sortKey="Trzeciakowski, Witold" uniqKey="Trzeciakowski W">Witold Trzeciakowski</name>
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<author><name sortKey="Majewski, Jacek A" uniqKey="Majewski J">Jacek A. Majewski</name>
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<term>Gallium Indium Arsenides Mixed</term>
<term>Gallium arsenides</term>
<term>High pressure</term>
<term>Laser diodes</term>
<term>Optical amplification</term>
<term>Pressure effects</term>
<term>Quantum well lasers</term>
<term>Temperature effects</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Effet pression</term>
<term>Diode laser</term>
<term>Laser puits quantique</term>
<term>Refroidissement</term>
<term>Haute pression</term>
<term>Effet température</term>
<term>Amplification optique</term>
<term>Gallium Indium Arséniure Mixte</term>
<term>Arséniure de gallium</term>
<term>InGaAs</term>
<term>GaAs</term>
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<front><div type="abstract" xml:lang="en">Wavelength dependent gain has been calculated for InGaAs/ GaAs quantum-well (QW) lasers as a function of hydrostatic pressure and temperature. The shift of the gain maximum for such laser is equal to -140 nm by increasing the pressure up to 20 kbar and -60 nm by cooling down from 300 to 100 K. The width of the gain curve (determining the possible tuning range with external grating) is significantly reduced at low temperatures and (to a lower extent) at high pressures. Our results indicate that pressure tuning is much more effective than temperature tuning when combined with tuning by external grating.</div>
</front>
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<fA08 i1="01" i2="1" l="ENG"><s1>Pressure and temperature dependence of gain in InGaAs/GaAs laser diode</s1>
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<fA11 i1="01" i2="1"><s1>BAJDA (Monika)</s1>
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<fA11 i1="02" i2="1"><s1>PIECHAL (Bernard)</s1>
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<fA11 i1="03" i2="1"><s1>DYBALA (Filip)</s1>
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<fA11 i1="04" i2="1"><s1>BERCHA (Artem)</s1>
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<fA11 i1="05" i2="1"><s1>TRZECIAKOWSKI (Witold)</s1>
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<fA11 i1="06" i2="1"><s1>MAJEWSKI (Jacek A.)</s1>
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<fA14 i1="01"><s1>Institute of Theoretical Physics, Faculty of Physics, University of Warsaw, Hoza 69</s1>
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<s3>POL</s3>
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<fA14 i1="02"><s1>Institute of High Pressure Physics, Polish Academy of Sciences, Sokolowska 29/37</s1>
<s2>01-142 Warszawa</s2>
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<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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<fA14 i1="03"><s1>Uzhgorod National University, Pidhirna 46</s1>
<s2>88000 Uzhgorod</s2>
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<fC01 i1="01" l="ENG"><s0>Wavelength dependent gain has been calculated for InGaAs/ GaAs quantum-well (QW) lasers as a function of hydrostatic pressure and temperature. The shift of the gain maximum for such laser is equal to -140 nm by increasing the pressure up to 20 kbar and -60 nm by cooling down from 300 to 100 K. The width of the gain curve (determining the possible tuning range with external grating) is significantly reduced at low temperatures and (to a lower extent) at high pressures. Our results indicate that pressure tuning is much more effective than temperature tuning when combined with tuning by external grating.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B40B55P</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Effet pression</s0>
<s5>02</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Pressure effects</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Diode laser</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Laser diodes</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Laser puits quantique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Quantum well lasers</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Refroidissement</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Cooling</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Haute pression</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>High pressure</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Effet température</s0>
<s5>07</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Temperature effects</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE"><s0>Amplification optique</s0>
<s5>11</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG"><s0>Optical amplification</s0>
<s5>11</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA"><s0>Amplificación óptica</s0>
<s5>11</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE"><s0>Gallium Indium Arséniure Mixte</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>12</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG"><s0>Gallium Indium Arsenides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>12</s5>
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<s2>NA</s2>
<s5>12</s5>
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<s2>NK</s2>
<s5>16</s5>
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<fC03 i1="09" i2="3" l="ENG"><s0>Gallium arsenides</s0>
<s2>NK</s2>
<s5>16</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>InGaAs</s0>
<s4>INC</s4>
<s5>52</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>GaAs</s0>
<s4>INC</s4>
<s5>53</s5>
</fC03>
<fN21><s1>030</s1>
</fN21>
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