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Two-dimensional coherent spectroscopy of trion-polaritons and exciton-polaritons in atomically thin transition metal dichalcogenides 原子薄过渡金属二掺杂化物中三离子-极坐标子和激子-极坐标子的二维相干光谱学
Pub Date : 2023-05-17 DOI: 10.1007/s43673-023-00081-8
Hui Hu, Jia Wang, Riley Lalor, Xia-Ji Liu

We present a microscopic many-body calculation of the nonlinear two-dimensional coherent spectroscopy (2DCS) of trion-polaritons and exciton-polaritons in charge-tunable transition-metal-dichalcogenides monolayers placed in an optical microcavity. The charge tunability leads to an electron gas with nonzero density that brings brightness to the trion — a polaron quasiparticle formed by an exciton with a nonzero residue bounded to the electron gas. As a result, a trion-polariton is created under strong light-matter coupling, as observed in the recent experiment by Sidler et al. [Nat. Phys. 13, 255 (2017)]. We analyze in detail the structure of trion-polaritons, by solving an extended Chevy ansatz for the trion quasiparticle wave-function. We confirm that the effective light-matter coupling for trion-polaritons is determined by the residue of the trion quasiparticle. The solution of the full many-body polaron states within Chevy ansatz enables us to microscopically calculate the nonlinear 2DCS spectrum of both trion-polaritons and exciton-polaritons. We predict the existence of three kinds of off-diagonal cross-peaks in the 2DCS spectrum, as an indication of the coherence among the different branches of trion-polaritons and exciton-polaritons. Due to the sensitivity of 2DCS spectrum to quasiparticle interactions, our work provides a good starting point to explore the strong nonlinearity exhibited by trion-polaritons in some recent exciton-polariton experiments.

我们介绍了对放置在光学微腔中的电荷可调谐过渡金属-二卤化物单层中的三离子-极化子和激子-极化子的非线性二维相干光谱(2DCS)的微观多体计算。电荷的可调谐性导致产生了密度非零的电子气,从而为三电子子带来了亮度--三电子子是一种由具有非零残余的激子形成的极子准粒子,与电子气结合在一起。因此,在强光-物质耦合作用下会产生三离子-极子,正如 Sidler 等人最近的实验所观察到的那样[Nat. Phys. 13, 255 (2017)]。我们通过求解三离子准粒子波函数的扩展切维解析式,详细分析了三离子-极化子的结构。我们证实,三离子-极坐标的有效光物耦合是由三离子准粒子的残余决定的。在切维解析中求解全多体极子态,使我们能够从微观上计算三离子-极子和激子-极子的非线性 2DCS 光谱。我们预测 2DCS 谱中存在三种非对角交叉峰,这表明三离子-极化子和激子-极化子的不同分支之间存在相干性。由于 2DCS 光谱对准粒子相互作用的敏感性,我们的工作为探索最近一些激子-极化子实验中三离子-极化子表现出的强非线性提供了一个良好的起点。
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引用次数: 0
Correction: News and Views (3&4) 更正:新闻与观点 (3&4)
Pub Date : 2023-05-09 DOI: 10.1007/s43673-023-00083-6
AAPPS Bulletin
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引用次数: 0
The development of active optical clock 有源光学时钟的发展
Pub Date : 2023-04-24 DOI: 10.1007/s43673-023-00079-2
Jia Zhang, Tiantian Shi, Jianxiang Miao, Jingbiao Chen

The atomic clocks, whether operating at optical or microwave region, can be divided into two categories according to their working mode, namely the passive clocks and active clocks. The passive clocks, whose standard frequency is locked to an ultra-narrow atomic spectral line, such as laser cooled Cs beam or lattice trapped Sr atoms, depend on the spontaneous emission line. On the contrary, the active clocks, in which the atoms are used as the gain medium, are based on the stimulated emission radiation, their spectrum can be directly used as the frequency standard. Up to now, the active hydrogen maser has been the most stable microwave atomic clocks. Also, the Sr superradiant active atomic clock is prospects for a millihertz-linewidth laser. Moreover, the optical clocks are expected to surpass the performance of microwave clocks both in stability and uncertainty, since their higher working frequency. The active optical clock has the potential to improve the stability of the best clocks by 2 orders of magnitude. In this work, we introduce the development of active optical clocks, and their types is classified according to the energy-level structure of atoms for stimulated radiation.

无论是工作在光学区还是微波区的原子钟,都可以根据其工作模式分为两类,即被动钟和主动钟。被动时钟的标准频率锁定在超窄原子谱线上,如激光冷却的铯束或晶格捕获的锶原子,其频率取决于自发辐射线。相反,以原子为增益介质的有源时钟则以受激发射辐射为基础,其光谱可直接用作频率标准。迄今为止,有源氢 maser 一直是最稳定的微波原子钟。同时,锶超辐射有源原子钟在毫赫兹线宽激光方面也具有广阔的前景。此外,由于工作频率较高,光学时钟有望在稳定性和不确定性方面超越微波时钟。有源光学时钟有可能将最佳时钟的稳定性提高两个数量级。在这项工作中,我们介绍了有源光学钟的发展,并根据受激辐射原子的能级结构对其类型进行了分类。
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引用次数: 0
News and Views (3&4) 新闻与观点 (3&4)
Pub Date : 2023-04-17 DOI: 10.1007/s43673-023-00078-3
AAPPS Bulletin
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引用次数: 0
All superconducting tokamak: EAST 所有超导托卡马克: EAST
Pub Date : 2023-04-11 DOI: 10.1007/s43673-023-00080-9
Jiansheng Hu, Weibin Xi, Jian Zhang, Liansheng Huang, Damao Yao, Qing Zang, Yanlan Hu, Guizhong Zuo, Qiping Yuan, Jinping Qian, Zhiwei Zhou, Xinjun Zhang, Mao Wang, Handong Xu, Yahong Xie, Zhengchu Wang, Haiqing Liu, Youwen Sun, Liang Wang, Guoqiang Li, Hongxing Yin, Yao Yang, Xianzu Gong, Kun Lu, Guosheng Xu, Junling Chen, Fukun Liu, Jiangang Li, Yuntao Song, the EAST team

Experimental Advanced Superconducting Tokamak (EAST) was built to demonstrate high-power, long-pulse operations under fusion-relevant conditions, with major radius R = 1.9 m, minor radius a = 0.5 m, and design pulse length up to 1000s. It has an ITER-like D-shaped cross-section with two symmetric divertors at the top and bottom, accommodating both single null and double null divertor configurations. EAST construction was started in 2000, and its first plasma was successfully obtained in 2006. In the past 15 years, plasma-facing components, plasma heating, diagnostics, and other systems have been upgraded step by step to meet its mission on exploring of the scientific and technological bases for fusion reactors and studying the physics and engineering technology issues with long pulse steady-state operation. An advanced steady-state plasma operation scenario has been developed, and plasma parameters were greatly improved. Meanwhile, front physics on the magnetic confinement plasmas have been systemically investigated and lots of fruitful results were realized, covering transport and confinement, MHD stabilities, pedestal physics, divertor and scrap-off layer (SOL) physics, and energetic particle physics. This brief review of EAST on engineering upgrading, stand-steady operation scenario development, and plasma physics investigation would be useful for the reference on construction and operation of a superconducting tokamak, such as ITER and future fusion reactor.

先进超导托卡马克实验装置(EAST)是为了在核聚变相关条件下演示大功率、长脉冲运行而建造的,其主要半径 R = 1.9 米,次要半径 a = 0.5 米,设计脉冲长度可达 1000 秒。它具有类似于热核聚变实验堆的 D 型横截面,顶部和底部有两个对称的分流器,可用于单空和双空分流器配置。EAST 于 2000 年开始建造,2006 年成功获得首个等离子体。在过去的15年中,面向等离子体的组件、等离子体加热、诊断和其他系统逐步升级,以满足其探索聚变反应堆的科学和技术基础以及研究长脉冲稳态运行的物理和工程技术问题的任务。开发了先进的稳态等离子体运行方案,等离子体参数得到极大改善。同时,对磁约束等离子体的前沿物理进行了系统研究,取得了大量丰硕成果,涵盖了输运与约束、MHD稳定性、基座物理、分流层和刮除层(SOL)物理以及高能粒子物理等方面。本文简要回顾了EAST在工程升级、稳态运行方案开发和等离子体物理研究方面的工作,对建造和运行超导托卡马克(如ITER和未来的聚变反应堆)具有参考价值。
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引用次数: 0
Recent progress on coherent computation based on quantum squeezing 基于量子挤压的相干计算最新进展
Pub Date : 2023-03-01 DOI: 10.1007/s43673-023-00077-4
Bo Lu, Lu Liu, Jun-Yang Song, Kai Wen, Chuan Wang

Squeezed vacuum state of light is an important concept of quantum optics which has an uncertainty reduction in a specific quadrature compared to the coherent vacuum state. The coherent Ising machines (CIMs) based on the squeezed state are capable of searching the ground state of the Ising model, which can be used to solve combinatorial optimization problems and have been experimentally demonstrated to have excellent computational performance. This review introduces the recent progress of a CIM hardware solver based on optical parametric oscillators, including the delayed optical path scheme and a measurement feedback scheme. Also, the basic principles, unique advantages, and potential challenges are described. We expect that the applications of large-scale CIM hardware solvers will have a huge impact on the acceleration of the computation power.

光的挤压真空态是量子光学的一个重要概念,与相干真空态相比,它的不确定性在特定的二次方中有所降低。基于挤压态的相干伊辛机(CIMs)能够搜索伊辛模型的基态,可用于解决组合优化问题,实验证明其具有优异的计算性能。本综述介绍了基于光参量振荡器的 CIM 硬件求解器的最新进展,包括延迟光路方案和测量反馈方案。此外,还介绍了基本原理、独特优势和潜在挑战。我们期待大规模 CIM 硬件求解器的应用将对加速计算能力产生巨大影响。
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引用次数: 0
News and views (1&2) 新闻和观点 (1&2)
Pub Date : 2023-02-16 DOI: 10.1007/s43673-023-00075-6
AAPPS Bulletin
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引用次数: 0
Squeezing for cosmic symphony 挤出宇宙交响乐
Pub Date : 2023-02-15 DOI: 10.1007/s43673-023-00076-5
Mengyao Wang, Fan Zhang

We briefly review the status of applying quantum squeezing to aid the search for gravitational waves with km-scale laser interferometers operating in the audio frequency band. The target audience is quantum optics professionals who are interested in an easily accessible introduction to the gravitational wave detector, both as an application of squeezing and as a platform for developing other quantum techniques.

我们简要回顾了应用量子挤压技术帮助在音频波段运行的千米级激光干涉仪搜索引力波的现状。我们的目标读者是量子光学专业人士,他们对引力波探测器的介绍很感兴趣,这既是量子挤压的应用,也是开发其他量子技术的平台。
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引用次数: 0
Ultrawide-bandgap semiconductor of carbon-based materials for meta-photonics-heterostructure, lasers, and holographic displays 碳基材料超宽带隙半导体用于元光子学--异质结构、激光器和全息显示器
Pub Date : 2023-01-27 DOI: 10.1007/s43673-022-00073-0
Arwa Saud Abbas

Carbon-based materials (CM) growth techniques include common growth factors for meta-photonics-heterostructure, holographic displays, and lasers. In this article, a review of basic growth using several sources is presented. The solid and gas sources of CVD and PLD techniques are discussed. Additionally, doping types and the fabrication of the CM devices are covered to satisfy the requirements of the light emitters’ functionality in the physics of materials as follows: (a) direct bandgap, (b) UV range of 0.1 μm < λG < 0.4 μm, 12.40 eV < EG > 3.10 eV, and (c) p-n junction formation. Additionally, conversion of injected electrical current into light in the semiconductor materials using the anti-electrons process for creating light emitters is proposed. Therefore, this review study explores the potential of the selected CM sources as an inexpensive and abundantly available renewable natural source for highly crystalline nanolayers. The CM status of epitaxial thin-film growth is introduced as well as device-processing technologies for prediction. Finally, the positron process in direct light conversion is discussed.

碳基材料(CM)生长技术包括元光子学(heterostructure)、全息显示和激光的常见生长因素。本文回顾了使用多种来源的基本生长技术。文章讨论了 CVD 和 PLD 技术的固体和气体源。此外,还介绍了 CM 器件的掺杂类型和制造方法,以满足以下材料物理中对发光体功能的要求:(a) 直接带隙,(b) 紫外范围 0.1 μm < λG < 0.4 μm,12.40 eV < EG > 3.10 eV,以及 (c) p-n 结的形成。此外,还提出了利用反电子过程在半导体材料中将注入的电流转化为光,从而产生发光体。因此,本综述研究探讨了所选 CM 源作为高结晶纳米层的廉价、丰富的可再生天然来源的潜力。此外,还介绍了外延薄膜生长的 CM 现状以及用于预测的设备加工技术。最后,讨论了直接光转换中的正电子过程。
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引用次数: 0
Coupling-selective quantum optimal control in weak-coupling NV-(^{13})C system 弱耦合 NV-(^{13})C 系统中的耦合选择性量子优化控制
Pub Date : 2023-01-05 DOI: 10.1007/s43673-022-00072-1
Feihao Zhang, Jian Xing, Xiaoxiao Hu, Xinyu Pan, Guilu Long

Quantum systems are under various unwanted interactions due to their coupling with the environment. Efficient control of quantum system is essential for quantum information processing. Weak-coupling interactions are ubiquitous, and it is very difficult to suppress them using optimal control method, because the control operation is at a time scale of the coherent life time of the system. Nitrogen-vacancy (NV) center of diamond is a promising platform for quantum information processing. The (^{13})C nuclear spins in the bath are weakly coupled to the NV, rendering the manipulation extremely difficulty. Here, we report a coupling selective optimal control method that selectively suppresses unwanted weak coupling interactions and at the same time greatly prolongs the life time of the wanted quantum system. We applied our theory to a 3 qubit system consisting of one NV electron spin and two (^{13})C nuclear spins through weak-coupling with the NV center. In the experiments, the iSWAP(^{dagger }) gate with selective optimal quantum control is implemented in a time-span of (T_{ctrl})= 170.25 (mu)s, which is comparable to the phase decoherence time (T_2)= 203 (mu s). The two-qubit controlled rotation gate is also completed in a strikingly 1020(80) (mu)s, which is five times of the phase decoherence time. These results could find important applications in the NISQ era.

量子系统由于与环境的耦合而受到各种不必要的相互作用。量子系统的有效控制对于量子信息处理至关重要。弱耦合相互作用无处不在,使用最优控制方法很难抑制它们,因为控制操作的时间尺度是系统的相干寿命。金刚石的氮空位(NV)中心是一个很有前景的量子信息处理平台。浴槽中(^{13})C核自旋与NV的耦合很弱,这给操作带来了极大的困难。在这里,我们报告了一种耦合选择性优化控制方法,它可以选择性地抑制不需要的弱耦合相互作用,同时大大延长所需的量子系统的寿命。我们将我们的理论应用于一个 3 量子位系统,该系统由一个 NV 电子自旋和两个 (^{13})C 核自旋通过与 NV 中心的弱耦合组成。在实验中,具有选择性最优量子控制的iSWAP({匕首})门实现的时间跨度为 (T_{ctrl})= 170.25 (mu)s,这与相位退相干时间 (T_2)= 203 (mu s)相当。双量子比特控制的旋转门也是在惊人的1020(80) (mu)s内完成的,是相位退相干时间的五倍。这些结果可以在NISQ时代找到重要的应用。
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