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首页> 外文期刊>IEEE journal of selected topics in quantum electronics >Pseudomorphic and Metamorphic Quantum Dot Heterostructures for Long-Wavelength Lasers on GaAs and Si
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Pseudomorphic and Metamorphic Quantum Dot Heterostructures for Long-Wavelength Lasers on GaAs and Si

机译:GaAs和Si上长波长激光器的伪和变质量子点异质结构

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摘要

We have investigated the design, molecular beam epitaxial growth, and fundamental characteristics of pseudomorphic and metamorphic quantum dot laser heterostructures on GaAs and Si. By utilizing the special techniques of low-temperature growth and in situ thermal annealing and carefully controlling various growth parameters, we have achieved 1.3–1.55-$mu$ m pseudomorphic and metamorphic quantum dot heterostructures on GaAs that exhibit superior optical quality. The special techniques of p-doping and tunnel injection have also been explored in the design and growth of quantum dot laser heterostructures, leading to long-wavelength lasers on GaAs that exhibit, for the first time, ultralow threshold current ($J_{rm th} = 63, {rm A}/{rm cm}^{2}$), nearly temperature-invariant operation ($T_{0} approx infty$), large modulation bandwidth ($f_{{-}{3,{rm dB}}} = 11, {rm GHz}$ ), near-zero $alpha$-parameter, and very small chirp (≦0.2 Å). With the incorporation of multiple layers of InAs quantum dots as effective three-dimensional dislocation filters, we have demonstrated the first room-temperature operational quantum dot lasers on Si that exhibit relatively low threshold current ($J_{rm th} = 900, {rm A}/{rm cm}^{2}$) and very high temperature stability ($T_{0} = 244, {rm K}$).
机译:我们研究了在GaAs和Si上的伪变质和变质量子点激光异质结构的设计,分子束外延生长以及基本特征。通过利用低温生长和原位热退火的特殊技术,并仔细控制各种生长参数,我们在GaAs上实现了1.3–1.55-μμm m的假晶和变质量子点异质结构,具有优异的光学质量。在量子点激光异质结构的设计和生长中,还探索了p掺杂和隧道注入的特殊技术,从而使GaAs上的长波长激光器首次展现出超低阈值电流($ J_ {rm th } = 63,{rm A} / {rm cm} ^ {2} $),几乎温度不变的操作($ T_ {0}约infty $),较大的调制带宽($ f _ {{{-} {3,{ rm dB}}} = 11,{rm GHz} $),接近零的$ alpha $参数和非常小的线性调频(≤0.2Å)。通过结合多层InAs量子点作为有效的三维位错滤光片,我们已经展示了Si上的第一批室温下工作的量子点激光器,该激光器具有相对较低的阈值电流($ J_ {rm th} = 900,{rm A} / {rm cm} ^ {2} $)和极高的温度稳定性($ T_ {0} = 244,{rm K} $)。

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