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  • 1
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 71, No. 16 ( 2022), p. 160303-
    Abstract: Hall tube is an important model to simulate the quantum Hall effect. However it hasn't been realized in superconducting circuits which have emerged as a promising platform for macro-controlling quantum effect. Taking advantage of the fine tunability of superconducting circuits, the three-chain superconducting transmon qubits with periodic boundary condition are designed in this paper. For constructing a synthetic Hall tube, ac magnetic fluxes are introduced to drive each transmon qubit. The gauge field emerged in this synthetic Hall tube can be tuned independently by properly choosing the driving phases. Then the ground-state chiral currents are discovered in this synthetic Hall tube, which are Meissner current on 〈inline-formula〉〈tex-math id="M1"〉\begin{document}$xy$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M1.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M1.png"/〉〈/alternatives〉〈/inline-formula〉 plane (〈inline-formula〉〈tex-math id="M2"〉\begin{document}$xy$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M2.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M2.png"/〉〈/alternatives〉〈/inline-formula〉-M), vortex current on 〈inline-formula〉〈tex-math id="M3"〉\begin{document}$xy$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M3.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M3.png"/〉〈/alternatives〉〈/inline-formula〉 plane (〈inline-formula〉〈tex-math id="M4"〉\begin{document}$xy$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M4.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M4.png"/〉〈/alternatives〉〈/inline-formula〉-V), vortex current on 〈inline-formula〉〈tex-math id="M5"〉\begin{document}$xz$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M5.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M5.png"/〉〈/alternatives〉〈/inline-formula〉 plane (〈inline-formula〉〈tex-math id="M6"〉\begin{document}$xz$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M6.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M6.png"/〉〈/alternatives〉〈/inline-formula〉-V), and vortex current on both 〈inline-formula〉〈tex-math id="M7"〉\begin{document}$xy$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M7.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M7.png"/〉〈/alternatives〉〈/inline-formula〉 and 〈inline-formula〉〈tex-math id="M8"〉\begin{document}$xz$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M8.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M8.png"/〉〈/alternatives〉〈/inline-formula〉 planes (DV). For distinguishing these chiral currents, four order parameters 〈inline-formula〉〈tex-math id="M9"〉\begin{document}$J_{C//}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M9.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M9.png"/〉〈/alternatives〉〈/inline-formula〉, 〈inline-formula〉〈tex-math id="M10"〉\begin{document}$J_{AB}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M10.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M10.png"/〉〈/alternatives〉〈/inline-formula〉 (〈inline-formula〉〈tex-math id="M11"〉\begin{document}$J_{BC}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M11.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M11.png"/〉〈/alternatives〉〈/inline-formula〉), and 〈inline-formula〉〈tex-math id="M12"〉\begin{document}$J_{CA}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M12.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M12.png"/〉〈/alternatives〉〈/inline-formula〉 are defined. Then the ground-state quantum phase diagrams are mapped out. The emergence of the different quantum phases is due to the competition between the coupling strengths 〈inline-formula〉〈tex-math id="M13"〉\begin{document}$\tilde{t}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M13.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M13.png"/〉〈/alternatives〉〈/inline-formula〉 and 〈inline-formula〉〈tex-math id="M14"〉\begin{document}$t_{CA}$\end{document}〈/tex-math〉〈alternatives〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M14.jpg"/〉〈graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="16-20220293_M14.png"/〉〈/alternatives〉〈/inline-formula〉. The Meissner and vortex currents emerging in this synthetic Hall tube also emerge in type II superconductor, which can generate an opposite field to weaken the influence of the applied field. Thus this synthetic Hall tube can be used as a diamagnet. At last we consider the influence of the imperfections in device fabrication. We proof when the strength of the imperfection is not large enough, the quantum phase diagrams shown in this paper remain valid. Moreover, the possible experimental observations of the ground-state chiral currents are addressed. The ground state of this synthetic Hall tube can be generated by applying microwave pulses. Then the corresponding density matrix can be constructed by the quantum state tomography. After constructing the density matrix, the order parameters can be obtained by calculating the trace. These results enrich the quantum currents in Hall tube and provide a new route to explore novel quantum phases.
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2022
    Location Call Number Limitation Availability
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  • 2
    Online Resource
    Online Resource
    Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences ; 2021
    In:  Acta Physica Sinica Vol. 70, No. 11 ( 2021), p. 114202-
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 70, No. 11 ( 2021), p. 114202-
    Abstract: Vertical cavity surface emitting lasers (VCSELs) have lots of excellent properties, such as circular beam, low threshold, single longitudinal mode, high speed modulation and monolithic array fabrication capability. The VCSELs have been widely used in data communication and short-distance optical interconnection. In the fields of distance detection and automatic driving, high accuracy lidars have become an indispensable component. In practical applications, 905 nm laser exhibits little absorption by the water vapor in the air. In addition, the 905 nm laser can match with both inexpensive Si detector and high response avalanche photodiode (APD). Therefore, the 905 nm semiconductor laser has become a key light source of lidar. This paper presents the design and fabrication of 905 nm VCSEL with high power conversion efficiency. First, the main factors influencing the power conversion efficiency (PCE) of VCSEL are analyzed theoretically. It is concluded that the slope efficiency contributes to the PCE most. In order to achieve a high slope efficiency, strained InGaAs is used as a quantum well material. Due to the wavelength redshift caused by the thermal effect, the lasing peak wavelength of the multiple quantum well (MQW) is designed to be about 892 nm by optimizing the In composition. The active region consists of three pairs of In〈sub〉0.123〈/sub〉Ga〈sub〉0.88〈/sub〉As/Al〈sub〉0.3〈/sub〉Ga〈sub〉0.7〈/sub〉 MQWs. The N-distributed Bragg reflectors (DBRs) are designed to have 40 pairs of Al〈sub〉0.9〈/sub〉Ga〈sub〉0.1〈/sub〉As/Al〈sub〉0.12〈/sub〉Ga〈sub〉0.88〈/sub〉As, and the P-DBRs are designed to have 20 pairs of Al〈sub〉0.9〈/sub〉Ga〈sub〉0.1〈/sub〉As/Al〈sub〉0.12〈/sub〉Ga〈sub〉0.88〈/sub〉As. The epitaxial structure is designed and grown by metal organic chemical vapor deposition (MOCVD). The cavity mode of the epitaxial wafer is around 903.7 nm. The photoluminescence (PL) spectrum is also measured. The peak wavelength is approximately 893.7 nm, and the full width at half maximum is 21.6 nm. Then, the 905 nm VCSELs with different apertures (6–18 μm) are fabricated via semiconductor technologies such as photolithography, evaporation, inductively coupled plasma (ICP), wet oxidation, electroplating, etc. Finally, the L-I-V characteristics and spectra of VCSELs with different apertures are tested. The obtained maximum slope efficiency and PCE of the devices are 1.12 W/A and 44.8%, respectively. In addition, the influences of aperture size on the far-field profiles and spectra of the devices are investigated. These 905 nm VCSELs with high PCE are potential for the miniaturization and lowing the cost of LiDAR.
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2021
    Location Call Number Limitation Availability
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  • 3
    Online Resource
    Online Resource
    Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences ; 2022
    In:  Acta Physica Sinica Vol. 71, No. 20 ( 2022), p. 204203-
    In: Acta Physica Sinica, Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences, Vol. 71, No. 20 ( 2022), p. 204203-
    Abstract: Aiming at three-dimensional (3D) sensing applications such as LiDAR, high power density five-junction cascaded vertical cavity surface emitting lasers (VCSELs) with 905 nm wavelength are designed and fabricated. The maximum power conversion efficiency is 55.2% for an individual VCSEL emitter with 8 μm oxide aperture. And the maximum slope efficiency of the device is 5.4 W/A, which is approximately 5 times that of traditional single-junction VCSEL with the same aperture. Under the condition of narrow pulse (pulse width 5.4 ns, duty cycle 0.019%) injection, the peak output power of 19-element array (20 μm oxidation aperture for each element) reaches 58.3 W, and the corresponding power density is as high as 1.62 kW/mm〈sup〉2〈/sup〉. The devices with various apertures (8–20 μm) are characterized. The results show that the maximum slope efficiencies of all these devices are greater than 5.4 W/A and the maximum PCE is higher than 54%. These high-performance VCSEL devices can be used as ideal light sources for 3D sensing applications such as LiDAR.
    Type of Medium: Online Resource
    ISSN: 1000-3290 , 1000-3290
    Language: Unknown
    Publisher: Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
    Publication Date: 2022
    Location Call Number Limitation Availability
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