Báo cáo hóa học: Spin effects in InAs self-assembled quantum dots
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Tuyển tập báo cáo các nghiên cứu khoa học quốc tế ngành hóa học dành cho các bạn yêu hóa học tham khảo đề tài: Spin effects in InAs self-assembled quantum dots
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Báo cáo hóa học: " Spin effects in InAs self-assembled quantum dots"dos Santos et al. Nanoscale Research Letters 2011, 6:115http://www.nanoscalereslett.com/content/6/1/115 NANO EXPRESS Open AccessSpin effects in InAs self-assembled quantum dotsEdnilson C dos Santos1, Yara Galvão Gobato1*, Maria JSP Brasil2, David A Taylor3, Mohamed Henini3 Abstract We have studied the polarized resolved photoluminescence in an n-type resonant tunneling diode (RTD) of GaAs/ AlGaAs which incorporates a layer of InAs self-assembled quantum dots (QDs) in the center of a GaAs quantum well (QW). We have observed that the QD circular polarization degree depends on applied voltage and light intensity. Our results are explained in terms of the tunneling of minority carriers into the QW, carrier capture by InAs QDs and bias-controlled density of holes in the QW.Introduction Our samples were processed into circular mesa structures of 400 μm diameter. A ring-shaped electricalResonant tunneling diodes (RTDs) are interestingdevices for spintronics because the spin character of the contact was used on the top of the mesa for opticalcarriers can be voltage selected [1-4]. Furthermore, spin access and PL and transport measurements under lightproperties of semiconductor quantum dots (QDs) are excitation. Magneto-transport and polarized resolved PLalso of high interest because electron spins can be used measurements were performed at 2 K under magneticas a quantum bit [5] for quantum computing [6] and fields up to 15 T parallel to the tunnel current by usingquantum communication [7]. In this paper, we have stu- an Oxford Magnet with optical window in the bottom.died spin polarization of carriers in resonant tunneling The measurements were performed by using a Prince-diodes with self-assembled InAs QD in the quantum ton InGaAs array diode system coupled with a singlewell region. The spin-dependent carrier transport along spectrometer. A linearly polarized line (514 nm) from an Ar+ laser was used for optical excitation. Therefore,the structure was investigated by measuring the left-and right-circularly polarized photoluminescence (PL) photogenerated carriers in the device do not present any preferential spin polarization degree. The right (s+)intensities from InAs QD and GaAs contact layers as a and left (s-) circularly polarized emissions were selectedfunction of the applied voltage, laser intensity and mag-netic fields up to 15 T. We have observed that the QD with appropriate optics (quarter wave plate andpolarization degree depends on bias and light intensity. polarizer).Our experimental results are explained by the tunneling Results and discussionof minority carriers into the quantum well (QW), carriercapture into the InAs QDs, carrier accumulation in the Figure 1 shows the schematic potential profile and car-QW region, and partial thermalization of minority rier dynamics in our device. Under applied bias voltage,carriers. electrons are injected from the GaAs emitter layer into Our devices were grown by molecular beam epitaxy on the QW region. Resonant tunneling condition isa n+ (001) GaAs substrate. The double-barrier structure obtained when the energy of carriers is equal to theconsists of two 8.3-nm Al0.4 Ga0.6 As barriers and a 12- energy of confined states in the QW. Under laser excita- tion, photogenerated holes tunnel through the QW andnm GaAs QW. A layer of InAs dots was grown in the can be captured by the QDs and eventually recombinecenter of the well by depositing 2.3 monolayers of InAs. radiatively. Carrier capture into QDs occurs within typi-Undoped GaAs spacer layer of width 50 nm separate theAl0.4 Ga0.6 As barriers from 2 × 1017 cm-3 n-doped GaAs cal times of about 1 ps which is much shorter than thelayers of width 50 nm. Finally, 3 × 10 18 cm -3 n-doped characteristic dwell times of electrons and holes that are tunneling resonantly into the QW. Due to this fast car-GaAs layers of width 0.3 nm were used to form contacts. rier capture process, the QD photoluminescence will be very sensitive to the r ...
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Báo cáo hóa học: " Spin effects in InAs self-assembled quantum dots"dos Santos et al. Nanoscale Research Letters 2011, 6:115http://www.nanoscalereslett.com/content/6/1/115 NANO EXPRESS Open AccessSpin effects in InAs self-assembled quantum dotsEdnilson C dos Santos1, Yara Galvão Gobato1*, Maria JSP Brasil2, David A Taylor3, Mohamed Henini3 Abstract We have studied the polarized resolved photoluminescence in an n-type resonant tunneling diode (RTD) of GaAs/ AlGaAs which incorporates a layer of InAs self-assembled quantum dots (QDs) in the center of a GaAs quantum well (QW). We have observed that the QD circular polarization degree depends on applied voltage and light intensity. Our results are explained in terms of the tunneling of minority carriers into the QW, carrier capture by InAs QDs and bias-controlled density of holes in the QW.Introduction Our samples were processed into circular mesa structures of 400 μm diameter. A ring-shaped electricalResonant tunneling diodes (RTDs) are interestingdevices for spintronics because the spin character of the contact was used on the top of the mesa for opticalcarriers can be voltage selected [1-4]. Furthermore, spin access and PL and transport measurements under lightproperties of semiconductor quantum dots (QDs) are excitation. Magneto-transport and polarized resolved PLalso of high interest because electron spins can be used measurements were performed at 2 K under magneticas a quantum bit [5] for quantum computing [6] and fields up to 15 T parallel to the tunnel current by usingquantum communication [7]. In this paper, we have stu- an Oxford Magnet with optical window in the bottom.died spin polarization of carriers in resonant tunneling The measurements were performed by using a Prince-diodes with self-assembled InAs QD in the quantum ton InGaAs array diode system coupled with a singlewell region. The spin-dependent carrier transport along spectrometer. A linearly polarized line (514 nm) from an Ar+ laser was used for optical excitation. Therefore,the structure was investigated by measuring the left-and right-circularly polarized photoluminescence (PL) photogenerated carriers in the device do not present any preferential spin polarization degree. The right (s+)intensities from InAs QD and GaAs contact layers as a and left (s-) circularly polarized emissions were selectedfunction of the applied voltage, laser intensity and mag-netic fields up to 15 T. We have observed that the QD with appropriate optics (quarter wave plate andpolarization degree depends on bias and light intensity. polarizer).Our experimental results are explained by the tunneling Results and discussionof minority carriers into the quantum well (QW), carriercapture into the InAs QDs, carrier accumulation in the Figure 1 shows the schematic potential profile and car-QW region, and partial thermalization of minority rier dynamics in our device. Under applied bias voltage,carriers. electrons are injected from the GaAs emitter layer into Our devices were grown by molecular beam epitaxy on the QW region. Resonant tunneling condition isa n+ (001) GaAs substrate. The double-barrier structure obtained when the energy of carriers is equal to theconsists of two 8.3-nm Al0.4 Ga0.6 As barriers and a 12- energy of confined states in the QW. Under laser excita- tion, photogenerated holes tunnel through the QW andnm GaAs QW. A layer of InAs dots was grown in the can be captured by the QDs and eventually recombinecenter of the well by depositing 2.3 monolayers of InAs. radiatively. Carrier capture into QDs occurs within typi-Undoped GaAs spacer layer of width 50 nm separate theAl0.4 Ga0.6 As barriers from 2 × 1017 cm-3 n-doped GaAs cal times of about 1 ps which is much shorter than thelayers of width 50 nm. Finally, 3 × 10 18 cm -3 n-doped characteristic dwell times of electrons and holes that are tunneling resonantly into the QW. Due to this fast car-GaAs layers of width 0.3 nm were used to form contacts. rier capture process, the QD photoluminescence will be very sensitive to the r ...
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