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Nonreciprocity of surface acoustic waves coupled to spin waves in a ferromagnetic bilayer with noncollinear layer magnetizations 具有非共线层磁化的铁磁双层中与自旋波耦合的表面声波的非互易性
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-19 DOI: 10.1103/physrevapplied.22.034046
Lidiia Ushii, Andrei Slavin, Roman Verba
Nonreciprocity of propagation of surface acoustic waves (SAWs) in the microwave frequency band can be achieved using the magnetoelastic interaction of SAWs with spin waves (SWs) propagating in magnetic heterostructures. Recent works have shown that the ultimate isolation of a counterpropagating hybridized SAW/SW is achieved in heterostructures consisting of a synthetic antiferromagnet—a ferromagnetic (FM) bilayer with antiferromagnetic Ruderman-Kittel-Kasuya-Yosida interlayer coupling—placed on top of a piezoelectric acoustic waveguide. In this work, we study in detail a more practical and technologically simpler system based on an FM bilayer, where layers are coupled by only dipole-dipole interaction, and having noncollinear magnetizations of the FM layers. A weak in-plane anisotropy with noncollinear easy axes in the layers is shown to be the only essential factor for the realization of strongly nonreciprocal propagation of a hybridized SAW/SW. We formulate requirements for the relative orientation of the layer’s magnetizations and wave propagation direction necessary to realize an efficient SAW isolator, and demonstrate examples of SAW transmission characteristics which prove the possibility of achieving an isolation exceeding 50 dB for a submillimeter-long FM bilayer with insertion losses of just a few decibels more than those of a pure SAW device. In addition to relative fabrication simplicity, the proposed magnetoelastic heterostructure exhibits a reasonable robustness in respect to deviations in the anisotropy axes and/or bias field directions—an important benefit for device mass production.
利用声表面波与在磁性异质结构中传播的自旋波(SW)之间的磁弹性相互作用,可以实现声表面波在微波频段的非互易传播。最近的研究表明,在由合成反铁磁体--具有反铁磁性 Ruderman-Kittel-Kasuya-Yosida 层间耦合的铁磁(FM)双层结构--放置在压电声波导顶部的异质结构中,可以实现反传播杂化 SAW/SW 的最终隔离。在这项工作中,我们详细研究了一个基于调频双电层的更实用、技术上更简单的系统,其中各层仅通过偶极-偶极相互作用耦合,并且调频层的磁化不共线。研究表明,各层中具有非共线易轴的微弱面内各向异性是实现混合声表面波/声表面波强非对等传播的唯一基本因素。我们提出了实现高效声表面波隔离器所需的层磁化相对方向和波传播方向的要求,并演示了声表面波传输特性的示例,证明亚毫米长的调频双层膜可以实现超过 50 dB 的隔离度,而插入损耗仅比纯声表面波器件高出几个分贝。除了相对简单的制造工艺外,所提出的磁弹性异质结构对各向异性轴和/或偏置场方向的偏差表现出合理的鲁棒性--这对器件的大规模生产具有重要的好处。
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引用次数: 0
Experimental demonstration of deep-learning-enabled adaptive optics 深度学习自适应光学实验演示
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-19 DOI: 10.1103/physrevapplied.22.034047
Hao-Bin Fu, Zu-Yang Wan, Yu-huai Li, Bo Li, Zhen Rong, Gao-Qiang Wang, Juan Yin, Ji-Gang Ren, Wei-Yue Liu, Sheng-Kai Liao, Yuan Cao, Cheng-Zhi Peng
Satellite-based quantum communication is a promising approach for establishing global-scale quantum networks. In free-space quantum channels, single-mode-fiber coupling plays a crucial role in increasing the signal-to-noise ratio of daylight quantum key distribution (QKD) and ensuring compatibility with standard fiber-based QKD protocols. However, consistently achieving high efficiency and stable single-mode-fiber coupling under strong atmospheric turbulence remains an ongoing experimental challenge. In this study, we experimentally demonstrate an adaptive method based on convolutional neural networks capable of directly estimating phase information from a single defocused image. We developed a convolutional neural network to establish the relationship between intensity distribution and phase information of turbulent distortions. We demonstrate the real-time performance of our deep-learning adaptive method in increasing single-mode-fiber coupling efficiency across various turbulence scales and quantify turbulence frequencies. Notably, the method proved highly effective in strong-turbulence scenarios, with frequencies reaching up to 200 Hz, leading to a significant increase in single-mode-fiber coupling efficiency. We demonstrate the corrective capability of our adaptive method for strong turbulence, enabled by the generalization of the convolutional neural network. Our results offer an efficient solution for daytime free-space QKD applications.
基于卫星的量子通信是建立全球规模量子网络的一种前景广阔的方法。在自由空间量子信道中,单模光纤耦合在提高日光量子密钥分发(QKD)的信噪比和确保与基于光纤的标准 QKD 协议兼容方面发挥着至关重要的作用。然而,在强大气湍流条件下持续实现高效稳定的单模光纤耦合仍然是一项持续的实验挑战。在本研究中,我们通过实验演示了一种基于卷积神经网络的自适应方法,该方法能够直接从单个散焦图像中估算相位信息。我们开发了一种卷积神经网络来建立湍流变形的强度分布和相位信息之间的关系。我们展示了深度学习自适应方法在提高各种湍流尺度的单模光纤耦合效率和量化湍流频率方面的实时性能。值得注意的是,该方法在强湍流情况下非常有效,频率高达 200 Hz,从而显著提高了单模光纤耦合效率。通过卷积神经网络的泛化,我们证明了自适应方法对强湍流的修正能力。我们的成果为日间自由空间 QKD 应用提供了高效的解决方案。
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引用次数: 0
Static quantum dot on a large potential hilltop for generating and analyzing hot electrons in the quantum Hall regime 大电势山顶上的静态量子点,用于产生和分析量子霍尔机制中的热电子
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-18 DOI: 10.1103/physrevapplied.22.034043
Ryo Oishi, Yuto Hongu, Tokuro Hata, Chaojing Lin, Takafumi Akiho, Koji Muraki, Toshimasa Fujisawa
We propose and demonstrate a static quantum dot on a potential hilltop to generate and analyze ballistic hot electrons along a quantum Hall edge channel well above the chemical potential. High-energy resolution associated with discrete energy levels is attractive for studying hot-electron dynamics. In particular, the energy distribution function of hot electrons weakly coupled to cold electrons is investigated to reveal spectral diffusion with energy relaxation. The analysis allows us to estimate the maximum energy exchange per scattering, which is a key parameter to describe interacting electrons in the edge channel.
我们提出并演示了一种静态量子点,该量子点位于化学势山顶,可沿着量子霍尔边缘通道产生并分析远高于化学势的弹道热电子。与离散能级相关的高能分辨率对于研究热电子动力学非常有吸引力。特别是,我们研究了与冷电子弱耦合的热电子的能量分布函数,以揭示能量弛豫的光谱扩散。通过分析,我们可以估算出每次散射的最大能量交换,这是描述边缘通道中相互作用电子的一个关键参数。
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引用次数: 0
Power-stabilized 3-W blue laser locked to the 420-nm transition in rubidium 锁定铷的 420 纳米转变的功率稳定的 3 瓦蓝色激光器
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-18 DOI: 10.1103/physrevapplied.22.034045
Jia Zhang, Xiaolei Guan, Xun Gao, Zhiyang Wang, Xiaomin Qin, Zijie Liu, Hangbo Shi, Jianxiang Miao, Tiantian Shi, Jingbiao Chen
Using modulation transfer spectroscopy, we achieve the frequency stabilization of a high-power 3-W blue laser at the wavelength of 420 nm to the <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mi>Rb</mi></math> <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>5</mn><msub><mi>S</mi><mrow><mn>1</mn><mo>/</mo><mn>2</mn></mrow></msub></math>–<math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>6</mn><msub><mi>P</mi><mrow><mn>3</mn><mo>/</mo><mn>2</mn></mrow></msub></math> transition. The in-loop frequency stability of this laser is <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>1.8</mn><mo>×</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>11</mn></mrow></msup><mo>/</mo><msqrt><mi>τ</mi></msqrt></math>, reaching <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>1.7</mn><mo>×</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>12</mn></mrow></msup></math> at 100 s and <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>7</mn><mo>×</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>13</mn></mrow></msup></math> at 1000 s. An external power feedback loop is established using an acousto-optic modulator, employing the zeroth-order diffracted light for power stabilization, achieving an in-loop power stability of <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>1.0</mn><mo>×</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>6</mn></mrow></msup></math> at 1 s. Moreover, the continuous mode-hop free interval of this high-power laser can simultaneously cover the <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>5</mn><msub><mi>S</mi><mrow><mn>1</mn><mo>/</mo><mn>2</mn></mrow></msub></math>–<math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mn>6</mn><msub><mi>P</mi><mrow><mn>3</mn><mo>/</mo><mn>2</mn></mrow></msub></math> transitions of <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi></mi><mn>85</mn></msup><mtext>Rb</mtext></math> and <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi></mi><mn>87</mn></msup><mtext>Rb</mtext></math>, with successful locking achieved for both isotopes, providing a comprehensive analysis of the <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><mi>Rb</mi></math> atomic transitions in the blue spectral region. As an application, this 3-W 420-nm laser with excellent power and frequency stabilities is used as a repumping source for diffuse laser cooling of <math display="inline" overflow="scroll" xmlns="http://www.w3.org/1998/Math/MathML"><msup><mi></mi><mn>87</mn></msup><mtext>Rb</mtext></math> atoms, realizing a one-meter-long cold-atom cloud. This paves the way for using blue-light cooling to realize a cold-<math disp
我们利用调制传递光谱技术,实现了波长为 420 nm 的高功率 3-W 蓝色激光器在掺铒 5S1/2-6P3/2 转变的频率稳定。利用声光调制器建立了外部功率反馈环路,利用零阶衍射光进行功率稳定,实现了 1.0×10-6 (1 s) 的环内功率稳定。此外,这种高功率激光器的连续无跳模间隔可同时覆盖 85Rb 和 87Rb 的 5S1/2-6P3/2 转变,并成功实现了对两种同位素的锁定,从而提供了对蓝谱区 Rb 原子转变的全面分析。在应用中,这台具有出色功率和频率稳定性的 3 瓦 420nm 激光器被用作 87Rb 原子扩散激光冷却的再泵浦源,实现了一米长的冷原子云。这为利用蓝光冷却实现冷掺铒原子主动光学时钟铺平了道路。此外,超高稳定的 420nm 激光还可应用于雷德堡原子实验、玻色-爱因斯坦凝聚、超窄带法拉第原子滤波器等多个领域。
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The in-loop frequency stability of this laser is &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn&gt;1.8&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;msqrt&gt;&lt;mi&gt;τ&lt;/mi&gt;&lt;/msqrt&gt;&lt;/math&gt;, reaching &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn&gt;1.7&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt; at 100 s and &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn&gt;7&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;13&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt; at 1000 s. An external power feedback loop is established using an acousto-optic modulator, employing the zeroth-order diffracted light for power stabilization, achieving an in-loop power stability of &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn&gt;1.0&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt; at 1 s. Moreover, the continuous mode-hop free interval of this high-power laser can simultaneously cover the &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;–&lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;msub&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;mo&gt;/&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt; transitions of &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msup&gt;&lt;mi&gt;&lt;/mi&gt;&lt;mn&gt;85&lt;/mn&gt;&lt;/msup&gt;&lt;mtext&gt;Rb&lt;/mtext&gt;&lt;/math&gt; and &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msup&gt;&lt;mi&gt;&lt;/mi&gt;&lt;mn&gt;87&lt;/mn&gt;&lt;/msup&gt;&lt;mtext&gt;Rb&lt;/mtext&gt;&lt;/math&gt;, with successful locking achieved for both isotopes, providing a comprehensive analysis of the &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mi&gt;Rb&lt;/mi&gt;&lt;/math&gt; atomic transitions in the blue spectral region. As an application, this 3-W 420-nm laser with excellent power and frequency stabilities is used as a repumping source for diffuse laser cooling of &lt;math display=\"inline\" overflow=\"scroll\" xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msup&gt;&lt;mi&gt;&lt;/mi&gt;&lt;mn&gt;87&lt;/mn&gt;&lt;/msup&gt;&lt;mtext&gt;Rb&lt;/mtext&gt;&lt;/math&gt; atoms, realizing a one-meter-long cold-atom cloud. This paves the way for using blue-light cooling to realize a cold-&lt;math disp","PeriodicalId":20109,"journal":{"name":"Physical Review Applied","volume":null,"pages":null},"PeriodicalIF":4.6,"publicationDate":"2024-09-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142248012","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Control of threshold voltages in Si/Si0.7Ge0.3 quantum devices via optical illumination 通过光学照明控制硅/硅 0.7Ge0.3 量子器件的阈值电压
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-18 DOI: 10.1103/physrevapplied.22.034044
M.A. Wolfe, Brighton X. Coe, Justin S. Edwards, Tyler J. Kovach, Thomas McJunkin, Benjamin Harpt, D.E. Savage, M.G. Lagally, R. McDermott, Mark Friesen, Shimon Kolkowitz, M.A. Eriksson
Optical illumination of quantum dot qubit devices at cryogenic temperatures, while not well studied, is often used to recover operating conditions after undesired shocking events or charge injection. Here, we demonstrate systematic threshold-voltage shifts in a dopant-free Si/Si0.7Ge0.3 field-effect transistor using a near-infrared (780-nm) laser diode. We find that illumination under an applied gate voltage can be used to set a specific, stable, and reproducible threshold voltage that, over a wide range in gate bias, is equal to that gate bias. Outside this range, the threshold voltage can still be tuned, although the resulting threshold voltage is no longer equal to the applied gate bias during illumination. We present a simple and intuitive model that provides a mechanism for the tunability in the gate bias. The model presented also explains why cryogenic illumination is successful at resetting quantum dot qubit devices after undesired charging events.
在低温条件下对量子点量子比特器件进行光学照明的研究虽然不多,但通常用于在意外冲击事件或电荷注入后恢复工作条件。在这里,我们利用近红外(780 纳米)激光二极管演示了无掺杂 Si/Si0.7Ge0.3 场效应晶体管的系统阈值电压偏移。我们发现,在施加的栅极电压下进行照明,可以设定一个特定、稳定和可重现的阈值电压,在很宽的栅极偏置范围内,阈值电压等于该栅极偏置。在此范围之外,阈值电压仍然可以调整,尽管由此产生的阈值电压不再等于照明时的外加栅极偏置。我们提出了一个简单直观的模型,为栅极偏置的可调谐性提供了一个机制。我们提出的模型还解释了为什么低温照明能在不希望发生的充电事件后成功重置量子点量子比特器件。
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引用次数: 0
Optically accelerated extreme learning machine using hot atomic vapors 利用热原子蒸汽的光学加速极端学习机
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-17 DOI: 10.1103/physrevapplied.22.034041
Pierre Azam, Robin Kaiser
Machine learning is becoming a widely used technique with impressive growth due to the diversity of problems of societal interest for which it can offer practical solutions. This increase of applications and required resources start to become limited by present-day hardware technologies. Indeed, novel machine learning subjects such as large language models or high-resolution image recognition raise the question of large computing time and energy cost of the required computation. In this context, optical platforms have been designed for several years with the goal of developing more efficient hardware for machine learning. Among different explored platforms, optical free-space propagation offers various advantages: parallelism, low energy cost, and computational speed. Here, we present a new design combining the strong and tunable nonlinear properties of a light beam propagating through a hot atomic vapor with an extreme learning machine model. We numerically and experimentally demonstrate the enhancement of the training using such free-space nonlinear propagation on an MNIST image classification task. We point out different experimental hyperparameters that can be further optimized to improve the accuracy of the platform.
机器学习正在成为一种广泛应用的技术,其增长速度令人印象深刻,这是因为它能为社会关注的各种问题提供实用的解决方案。应用和所需资源的增加开始受到当今硬件技术的限制。事实上,大型语言模型或高分辨率图像识别等新型机器学习课题都提出了所需计算时间长、能耗高的问题。在这种情况下,人们多年来一直在设计光学平台,目的是为机器学习开发更高效的硬件。在已探索的各种平台中,自由空间光学传播具有并行性、低能耗成本和计算速度等多种优势。在这里,我们提出了一种新的设计,它将在热原子蒸汽中传播的光束的强可调非线性特性与极端学习机模型相结合。我们通过数值和实验证明,在 MNIST 图像分类任务中使用这种自由空间非线性传播技术可以增强训练效果。我们指出了可以进一步优化的不同实验超参数,以提高平台的准确性。
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引用次数: 0
Spin-orbit-locked coupling of localized microwaves to magnons 局部微波与磁子的自旋轨道锁定耦合
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-17 DOI: 10.1103/physrevapplied.22.034042
Chengyuan Cai, Zubiao Zhang, Ji Zou, Gerrit E. W. Bauer, Tao Yu
We address the photonic spin-orbit coupling known from nano-optics and plasmonics in the microwave regime. The spin S and momentum q of microwaves emitted by an excited magnetic particle are locked by qS=0 with a fixed chirality n^(S^×q^)=1 when evanescent along n^q. This field excites magnons in a nearby magnetic film in the form of directional beams that rotate with the magnetization direction. The exchange of these magnons between two distant nanomagnets leads to a highly tunable strong coupling and entangles their excited states.
我们探讨了微波体系中纳米光学和等离子体学中已知的光子自旋轨道耦合。受激磁性粒子发射的微波的自旋 S 和动量 q 被 q⋅S=0 锁定,当沿 n^⊥q 蒸发时,具有固定的手性 n^⋅(S^×q^)=1。这个磁场会在附近的磁性薄膜中激发出磁子,这些磁子以定向束的形式随磁化方向旋转。这些磁子在两个相距甚远的纳米磁体之间的交换导致了高度可调的强耦合,并使它们的激发态纠缠在一起。
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引用次数: 0
Toolbox for nonreciprocal dispersive models in circuit quantum electrodynamics 电路量子电动力学非互易色散模型工具箱
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-16 DOI: 10.1103/physrevapplied.22.034038
Lautaro Labarca, Othmane Benhayoune-Khadraoui, Alexandre Blais, Adrian Parra-Rodriguez
We provide a systematic method for constructing effective dispersive Lindblad master equations to describe weakly anharmonic superconducting circuits coupled by a generic dissipationless nonreciprocal linear system, with effective coupling parameters and decay rates written in terms of the immittance parameters characterizing the coupler. This article extends the foundational work of Solgun et al. [IEEE Trans. Microw. Theory Techn. 67, 928 (2019)] for linear reciprocal couplers described by an impedance response. Notably, we expand the existing toolbox to incorporate nonreciprocal elements, account for direct stray coupling between immittance ports, circumvent potential singularities, and include collective dissipative effects that arise from interactions with external common environments. We illustrate the use of our results with a circuit of weakly anharmonic Josephson junctions coupled to a multiport nonreciprocal environment and a dissipative port. The results obtained here can be used for the design of complex superconducting quantum processors with nontrivial routing of quantum information, as well as analog quantum simulators of condensed matter systems.
我们提供了一种构建有效色散林德布拉德主方程的系统方法,以描述由通用无耗散非互易线性系统耦合的弱非谐波超导电路,其有效耦合参数和衰减率用表征耦合器的惰性参数来表示。本文扩展了 Solgun 等人 [IEEE Trans. Microw. Theory Techn.值得注意的是,我们扩展了现有的工具箱,纳入了非互易元素,考虑了互易端口之间的直接杂散耦合,规避了潜在的奇异性,并包含了与外部共同环境相互作用产生的集体耗散效应。我们用一个与多端口非互易环境和耗散端口耦合的弱非谐波约瑟夫森结电路来说明我们的结果的用途。这里获得的结果可用于设计复杂的超导量子处理器与量子信息的非线性路由,以及凝聚态系统的模拟量子模拟器。
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引用次数: 0
Unidirectional spin waves measured using propagating-spin-wave spectroscopy 利用传播自旋波光谱学测量单向自旋波
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-16 DOI: 10.1103/physrevapplied.22.034040
G.Y. Thiancourt, S.M. Ngom, N. Bardou, T. Devolder
The dispersion relation of spin waves can vary monotonically about the center of the Brillouin zone, allowing zero-momentum wavepackets to flow unidirectionally, which is of interest for applications. Techniques such as propagating-spin-wave spectroscopy are inoperative in such cases because of the difficulty to identify the spin-wave wavevector at a particular frequency within a spectrum. Here we present a method to analyze this case and apply it to acoustic spin waves in a synthetic antiferromagnet in the scissors state, in which we confirm that propagation parallel to the applied fields is unidirectional. Interestingly, we find that in this unidirectional situation, the phase accumulated by the spin waves propagating between two antennas is not proportional to the antenna spacing. It is also a function of the two other lengths of the problem: the antenna width and the spin-wave decay length. Accounting for them is required to avoid wavevector errors in the dispersion relations.
自旋波的色散关系可围绕布里渊区中心单调变化,允许零动量波包单向流动,这在应用中很有意义。在这种情况下,传播自旋波光谱学等技术无法发挥作用,因为很难在光谱中识别特定频率的自旋波波向。在这里,我们提出了一种分析这种情况的方法,并将其应用于处于剪刀态的合成反铁磁体中的声学自旋波,在这种情况下,我们证实平行于外加磁场的传播是单向的。有趣的是,我们发现在这种单向情况下,在两个天线之间传播的自旋波累积的相位与天线间距并不成正比。它还是问题中另外两个长度的函数:天线宽度和自旋波衰减长度。要避免频散关系中的波矢误差,就必须考虑到这两个因素。
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引用次数: 0
Shrinking a gradient-index-lens antenna system with a spaceplate 用空间板缩小梯度指数透镜天线系统
IF 4.6 2区 物理与天体物理 Q2 PHYSICS, APPLIED Pub Date : 2024-09-16 DOI: 10.1103/physrevapplied.22.034039
Michal Mrnka, Thomas Whittaker, David B. Phillips, Euan Hendry, Will Whittow
The miniaturization of optical systems is an ongoing challenge across the electromagnetic spectrum. While the thickness of optical elements themselves can be reduced using advances in metamaterials, it is the voids between these elements—which are necessary parts of an optical system—that occupy most of the volume. Recently, a novel optical element coined a “spaceplate” has been proposed, which replaces a region of free space with a thinner optical element that emulates the free-space optical response function—thus having the potential to substantially shrink the volume of optical systems. While there have been a few proof-of-principle demonstrations of spaceplates, they have not yet been deployed in a real-world optical system. In this work, we use a bespoke-designed spaceplate to reduce the length of a gradient-index- (GRIN) lens microwave antenna. Our antenna is designed to operate at 23.5 GHz and the incorporation of a nonlocal metamaterial spaceplate enables the distance between the antenna feed and the GRIN lens to be reduced by almost a factor of 2. We find that the radiation patterns from a conventional and space-squeezed antenna are very similar, with a very low cross-polarization, and only a minor increase in the side-lobe levels when introducing the spaceplate. Our work represents a demonstration of a spaceplate integrated into a real-world optical system operating in microwave spectral region, highlighting the potential for this concept to reduce the physical size of systems in applications including imaging, spectroscopy, radar, and communications.
光学系统的微型化是整个电磁频谱领域一直面临的挑战。虽然超材料技术的发展可以减小光学元件本身的厚度,但占据大部分体积的却是这些元件之间的空隙--它们是光学系统的必要组成部分。最近,一种被称为 "空间板 "的新型光学元件被提出,这种光学元件用更薄的光学元件取代了自由空间区域,模拟了自由空间的光学响应功能,因此有可能大幅缩小光学系统的体积。虽然已经有一些空间板的原理验证演示,但它们尚未在实际光学系统中部署。在这项工作中,我们使用定制设计的空间板来缩短梯度指数(GRIN)透镜微波天线的长度。我们发现,传统天线和空间挤压天线的辐射模式非常相似,交叉极化非常低,引入空间板后侧叶水平仅略有增加。我们的工作是将空间板集成到在微波频谱区工作的实际光学系统中的一次演示,凸显了这一概念在缩小成像、光谱学、雷达和通信等应用系统的物理尺寸方面的潜力。
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引用次数: 0
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Physical Review Applied
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