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Probe absorption characteristics and Kerr effect of a hybrid phonon-spin-magnon system 声子-自旋-磁子混合系统的探针吸收特性和克尔效应
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-08-18 DOI: 10.1140/epjd/s10053-024-00896-6
Qing-hong Liao, Chen-ting Deng, Hai-yan Qiu

We theoretically explore the absorption spectra and Kerr effect of a phonon-spin-magnon hybrid system, in which the nitrogen-vacancy (NV) center is coupled with a yttrium iron garnet (YIG) crystal and a mechanical resonator simultaneously. The results indicate that vacuum Rabi splitting can occur in the absorption spectrum by modulating the coupling strength between the YIG sphere and the NV center. We show the vacuum Rabi splitting and the transparency based on mechanically induced coherent population oscillation (MICPO) to be adjusted by the decay rate of the YIG sphere and the mechanical resonator, respectively. Moreover, it is indicated the absorption spectra can be flexibly tuned by changing the frequency tuning of the spin-pump field. Furthermore, the nonlinear Kerr effect is controllable via varying the Rabi frequency. The study could provide a way for general applications in quantum computing devices and quantum information processing.

Graphical abstract

我们从理论上探讨了声子-自旋-磁子混合系统的吸收光谱和克尔效应,在该系统中,氮空位(NV)中心同时与钇铁石榴石(YIG)晶体和机械谐振器耦合。结果表明,通过调节 YIG 球和 NV 中心之间的耦合强度,可以在吸收光谱中产生真空拉比分裂。我们表明,真空拉比分裂和基于机械诱导相干群体振荡(MICPO)的透明度可分别通过 YIG 球和机械谐振器的衰减率来调节。此外,研究还表明,通过改变自旋泵场的频率调节,可以灵活地调整吸收光谱。此外,非线性克尔效应也可以通过改变拉比频率来控制。这项研究可为量子计算设备和量子信息处理的普遍应用提供一种途径。 图文摘要
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引用次数: 0
R-matrix with time-dependence calculations for three-sideband RABBITT in helium 氦气中三边带 RABBITT 的 R 矩阵与时间相关性计算
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-08-14 DOI: 10.1140/epjd/s10053-024-00900-z
A. T. Bondy, J. C. del Valle, S. Saha, K. R. Hamilton, D. Bharti, A. Harth, K. Bartschat

Following up on a recent paper (Bharti et al. in Phys Rev A 109:023110, 2024), we compare the predictions from several R-matrix with time-dependence calculations for a modified three-sideband version of the “reconstruction of attosecond beating by interference of two-photon transitions” (RABBITT) configuration applied to helium. Except for the special case of the threshold sideband, which appears to be very sensitive to the details of coupling to the bound Rydberg states, increasing the number of coupled states in the close-coupling expansion used to describe the ejected-electron–residual-ion interaction hardly changes the results. Consequently, the remaining discrepancies between the experimental data and the theoretical predictions are likely due to uncertainties in the experimental parameters, particularly the detailed knowledge of the laser pulse.

摘要继最近的一篇论文(Bharti 等人,Phys Rev A 109:023110, 2024)之后,我们比较了几种 R 矩阵的预测结果,以及应用于氦的 "双光子跃迁干涉重建阿秒跳动"(RABBITT)配置的修正三边带版本的时间相关性计算结果。除了阈值边带的特殊情况外(阈值边带似乎对与束缚雷德贝格态耦合的细节非常敏感),在用于描述射出电子-残余离子相互作用的紧密耦合扩展中,增加耦合态的数量几乎不会改变结果。因此,实验数据与理论预测之间的其余差异很可能是由于实验参数的不确定性造成的,特别是对激光脉冲的详细了解。
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引用次数: 0
Radiative and opacity data obtained from large-scale atomic structure calculations and from statistical simulations for the spectral analysis of kilonovae in their photospheric and nebular phases: the sample case of Er III 通过大规模原子结构计算和统计模拟获得的用于光球和星云阶段千新星光谱分析的辐射和不透明度数据:Er III 的样本案例
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-08-13 DOI: 10.1140/epjd/s10053-024-00897-5
Jérôme Deprince, Helena Carvajal Gallego, Sirine Ben Nasr, Lucas Maison, Jean-Christophe Pain, Patrick Palmeri, Pascal Quinet

This study is an overview of the atomic data and opacity computations performed by the Atomic Physics and Astrophysics Unit of Mons University in the context of kilonova emission following neutron star mergers, in both the photospheric and nebular phases. In this work, as a sample case, we focus on a specific lanthanide ion, namely Er III. As far as the LTE photospheric phase of the kilonova ejecta is concerned, we present our calculations using both a theoretical method (the pseudo-relativistic Hartree-Fock method, HFR) and a statistical approach (the Resolved Transition Array approach, RTA) to obtain the atomic data required to estimate the Er III expansion opacity for typical conditions expected in kilonova ejecta one day after the merger. In order to draw the limitations of both of our strategies, the results obtained using the latter are compared, and a calibration procedure of the HFR atomic data in this context is also discussed. Concerning the kilonova ejecta nebular phase, atomic parameters that characterize forbidden lines in Er III are calculated using HFR as well as another computational approach, namely the Multiconfiguration Dirac–Hartree–Fock (MCDHF) method. The potential detection of such lines in late-phase kilonova spectra is then discussed.

摘要 本研究综述了蒙斯大学原子物理学和天体物理学研究组在中子星合并后的千新星发射背景下,在光球和星云阶段所进行的原子数据和不透明度计算。在这项研究中,我们以一种特定的镧系离子(即 Er III)为样本。就千新星喷出物的LTE光球阶段而言,我们使用理论方法(伪相对论哈特里-福克方法,HFR)和统计方法(分辨转换阵列方法,RTA)进行了计算,以获得所需的原子数据,从而估算出合并后一天的千新星喷出物在典型条件下的Er III膨胀不透明度。为了说明我们这两种方法的局限性,对使用后者得到的结果进行了比较,并讨论了在这种情况下对高频原子数据的校准程序。关于千新星喷出星云阶段,使用氢FR和另一种计算方法,即多配置狄拉克-哈特里-福克(MCDHF)方法,计算了表征 Er III 中禁止线的原子参数。然后讨论了在晚期千新星光谱中探测到这些线的可能性。
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引用次数: 0
High precision in a Fourier-transform spectrum of protactinium: extensive weighted least-squares fits of peak wavenumbers for analysis of fine and hyperfine structure 镤的傅立叶变换光谱的高精度:用于分析精细和超精细结构的峰值文数的广泛加权最小二乘法拟合
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-08-13 DOI: 10.1140/epjd/s10053-024-00895-7
Sophie Kröger
<p>A Fourier-transform recording of protactinium in the infrared range is reanalysed with high precision in order to determine the hyperfine interaction constants <i>A</i> and <i>B</i>. Starting with a selection of best lines and least-squares fits of hyperfine structure intervals, large systems of linear equations compare experimental hyperfine peak wavenumbers with a theoretical representation. The theoretical representation is based on Ritz’s combination principle and Casimir’s formula according to the existing classification. Weighted least-squares fits allow a discrimination between unperturbed and perturbed data such as blended hyperfine structure components. For the first time, the wavenumbers of the hyperfine components of more than 600 lines are fitted using the characteristics of about 250 levels as parameters. When adding adjustable wavenumber-scale correction parameters, global consistency for the whole IR spectrum is obtained with local limits of about <span>(0.3,times 10^{-3})</span> cm<span>(^{-1})</span>. This demonstrates the high precision in both recording and analysis. The values of the fine structure energies are revised. Standard errors around 0.1 <span>(times 10^{-3})</span> cm<span>(^{-1})</span> for the <i>A</i> constants and 10<span>(^{-3})</span> cm<span>(^{-1})</span> for the <i>B</i> constants and the fine structure energies are achieved. Representative examples illustrate extensive results obtained for atomic protactinium. This high precision facilitates further search for new energy levels, and 20 new levels were presented. <b>Foreword</b> The data presented here are the results of a study carried out at the Laboratoire Aimé Cotton (LAC) at Paris-Orsay in the years 2003 and 2004, when I was there for a research stay. At this time, I worked together with Jean-François Wyart and Annie Ginibre on the re-examination of protactinium spectra that have been measured about 30 years earlier and that were available in the form of a printed list of peak wavenumbers and a printed paper chart of the intensity profile. The spectra had already been analysed, but there was still a lot of additional information that could be extracted from the spectra with time and effort. The review of the data, the selection of the data and the step-by-step optimization of the data set took a lot of time. When I returned to Berlin in 2004, we had made good progress, but in principle, it is like a bottomless pit. We continued together to optimize the data and tried to the finishing touches to it. At some point, we decided that we had reached a ‘level of maturity’ where the data could be published. We have discussed a lot about how detailed the text should be. This discussion has dragged on over the years and this project has repeatedly been lost in the stream of other everyday tasks. Every now and then there was a small attempt to return to this topic, but it quickly got lost in the daily hustle and bustle. In 2012, we presented the results at a co
摘要 为了确定超正弦相互作用常数 A 和 B,对质子在红外范围内的傅立叶变换记录进行了高精度的重新分析。根据现有的分类,理论表示是基于里兹组合原理和卡西米尔公式。加权最小二乘法拟合可以区分未扰动数据和扰动数据,如混合超正弦结构成分。首次使用大约 250 个层次的特征作为参数,拟合了 600 多条谱线的超正弦成分的文波数。当添加可调节的文波数尺度校正参数时,整个红外光谱获得了全局一致性,局部极限约为(0.3,times 10^{-3}) cm(^{-1}) 。这表明记录和分析的精度都很高。精细结构能量的值是经过修正的。A 常量的标准误差约为 0.1 (乘以 10^{-3}) cm(^{-1}) ,B 常量和精细结构能的标准误差约为 10(^{-3}) cm(^{-1}) 。有代表性的例子说明了原子镤的广泛结果。这种高精度有助于进一步寻找新能级,并提出了 20 个新能级。前言 本文介绍的数据是我于 2003 年和 2004 年在巴黎奥赛艾梅-科顿实验室(LAC)进行研究的结果。当时,我与让-弗朗索瓦-怀亚特(Jean-François Wyart)和安妮-吉尼布雷(Annie Ginibre)合作,对大约 30 年前测量的镤化物光谱进行了重新研究。虽然已经对光谱进行了分析,但仍有许多额外的信息可以通过花费时间和精力从光谱中提取出来。审查数据、选择数据和逐步优化数据集花费了大量时间。2004 年我回到柏林时,我们已经取得了不错的进展,但原则上,这就像一个无底洞。我们继续一起优化数据,并试图对其进行收尾工作。在某个阶段,我们认为我们已经达到了可以公布数据的 "成熟度"。我们就文本的详细程度进行了多次讨论。这种讨论拖了好几年,这个项目也一再被其他日常工作淹没。时不时地,我们会尝试回到这个话题,但很快就会被日常的喧嚣所淹没。2012 年,我们在一次会议上展示了研究成果。他们两人在两年内相继去世,这对我打击很大。我非常遗憾这项工作未能尽早出版。这本特辑是我最终发表这些数据的正确动力。我现在既无法获得当时在大型计算机系统上运行的计算机程序,也无法获得原始测量数据。我也无法找到大量的纸张(峰值波数的打印列表和光谱的打印纸质图表)的去向。但我有一堆计算的输入和输出文件,这些文件多年来已变得有些杂乱,其中包含大量信息,还有我们未完成的手稿。由此产生的数据包含了对后人很重要的信息--尤其是因为该元素具有放射性,而收集实验室数据的实验在短期内不太可能重复。我认为值得公布这些数据。图文摘要Pa 的高精度傅立叶变换光谱:精细和超精细结构分析
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引用次数: 0
Spectral phase pulse shaping reduces ground state depletion in high-order harmonic generation 频谱相位脉冲整形可减少高阶谐波产生过程中的基态损耗
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-08-13 DOI: 10.1140/epjd/s10053-024-00890-y
J. Aygun, C. G. Buitrago, M. F. Ciappina, A. L. Harris

High-order harmonic generation (HHG) has become an indispensable process for generating attosecond pulse trains and single attosecond pulses used in the observation of nuclear and electronic motion. As such, improved control of the HHG process is desirable, and one such possibility for this control is through the use of structured laser pulses. We present numerical results from solving the one-dimensional time-dependent Schrödinger equation for HHG from hydrogen using Airy and Gaussian pulses that differ only in their spectral phase. Airy pulses have identical power spectra to Gaussian pulses, but different spectral phases and temporal envelopes. We show that the use of Airy pulses results in less ground state depletion compared to the Gaussian pulse, while maintaining harmonic yield and cutoff. Our results demonstrate that Airy pulses with higher intensity can produce similar HHG spectra to lower intensity Gaussian pulses without depleting the ground state. The different temporal envelopes of the Gaussian and Airy pulses lead to changes in the dynamics of the HHG process, altering the time-dependence of the ground state population and the emission times of the high harmonics.

Graphical abstract

High-order harmonic generation (HHG) using an Airy pulse with a third order spectral phase results in less ground state depletion, but similar harmonic yield, compared to a Gaussian pulse. Top – schematic depiction of the 3-step HHG process for different intensity pulses. Bottom left – time-dependent ground state populations for Gaussian pulses showing that a more intense pulse causes more ground state depletion. Bottom middle – final ground state populations for Airy and Gaussian pulses as a function of intensity showing that Airy pulses result in less ground state depletion for a given intensity. Bottom right – HHG spectra for a more intense Airy pulse and a less intense Gaussian pulse exhibit similar shapes, magnitudes, and plateau cutoff values

高阶谐波发生(HHG)已成为产生用于观测核运动和电子运动的阿秒脉冲串和单个阿秒脉冲不可或缺的过程。因此,我们希望改进对 HHG 过程的控制,其中一种控制方法是使用结构化激光脉冲。我们介绍了使用Airy脉冲和高斯脉冲求解氢的一维时变薛定谔方程的数值结果。Airy脉冲与高斯脉冲具有相同的功率谱,但光谱相位和时间包络不同。我们的研究结果表明,与高斯脉冲相比,使用Airy脉冲可减少基态损耗,同时保持谐波产量和截止。我们的结果表明,强度较高的空气脉冲可以产生与强度较低的高斯脉冲类似的 HHG 光谱,而不会损耗基态。高斯脉冲和Airy脉冲的不同时间包络导致了HHG过程的动态变化,改变了基态种群的时间依赖性和高次谐波的发射时间。
{"title":"Spectral phase pulse shaping reduces ground state depletion in high-order harmonic generation","authors":"J. Aygun,&nbsp;C. G. Buitrago,&nbsp;M. F. Ciappina,&nbsp;A. L. Harris","doi":"10.1140/epjd/s10053-024-00890-y","DOIUrl":"10.1140/epjd/s10053-024-00890-y","url":null,"abstract":"<div><p>High-order harmonic generation (HHG) has become an indispensable process for generating attosecond pulse trains and single attosecond pulses used in the observation of nuclear and electronic motion. As such, improved control of the HHG process is desirable, and one such possibility for this control is through the use of structured laser pulses. We present numerical results from solving the one-dimensional time-dependent Schrödinger equation for HHG from hydrogen using Airy and Gaussian pulses that differ only in their spectral phase. Airy pulses have identical power spectra to Gaussian pulses, but different spectral phases and temporal envelopes. We show that the use of Airy pulses results in less ground state depletion compared to the Gaussian pulse, while maintaining harmonic yield and cutoff. Our results demonstrate that Airy pulses with higher intensity can produce similar HHG spectra to lower intensity Gaussian pulses without depleting the ground state. The different temporal envelopes of the Gaussian and Airy pulses lead to changes in the dynamics of the HHG process, altering the time-dependence of the ground state population and the emission times of the high harmonics.</p><h3>Graphical abstract</h3><div><figure><div><div><picture><source><img></source></picture></div><div><p>High-order harmonic generation (HHG) using an Airy pulse with a third order spectral phase results in less ground state depletion, but similar harmonic yield, compared to a Gaussian pulse. Top – schematic depiction of the 3-step HHG process for different intensity pulses. Bottom left – time-dependent ground state populations for Gaussian pulses showing that a more intense pulse causes more ground state depletion. Bottom middle – final ground state populations for Airy and Gaussian pulses as a function of intensity showing that Airy pulses result in less ground state depletion for a given intensity. Bottom right – HHG spectra for a more intense Airy pulse and a less intense Gaussian pulse exhibit similar shapes, magnitudes, and plateau cutoff values</p></div></div></figure></div></div>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"78 8","pages":""},"PeriodicalIF":1.5,"publicationDate":"2024-08-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjd/s10053-024-00890-y.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196122","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Interference and tunneling of beams in fractional systems with rectangular potential 具有矩形势能的分数系统中光束的干涉和隧道效应
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-08-10 DOI: 10.1140/epjd/s10053-024-00901-y
Min Han, Xiaoqin Bai, Rongcao Yang

The dynamics of hyperbolic secant beams under the competition between the fractional diffraction and rectangular potential is investigated. It is found that the beams can exhibit the reflection, tunneling and interference, forming the bound states, optical lattices or fringes, or solitons under different conditions. In linear regime, when the potential is wide, the beam exhibits the total reflection for deeper potential and smaller incident angle, and presents the reflection and tunneling for shallower potential and larger incident angle. The irregular interference pattern and bound states are generated for the narrow potential. Moreover, the initial chirp causes the appearance of side lobes during beam propagation. When two hyperbolic secant beams are symmetrically incident from inside or outside the potential, the interference lattices or interference fringes are generated inside the potential, which are related to the Lévy index, initial chirp and incident angle of the beams. In nonlinear regime, the hyperbolic secant beam undergoes the collapse, splitting or formation of the periodic-like soliton by selecting appropriate parameters including the Lévy index, initial chirp and incident angle. In addition, the dynamics of two hyperbolic secant beams under the interaction of the nonlinear effect and fractional diffraction is also investigated in detail. This work provides more possibilities for optical lattice generation and optical manipulation.

Graphical abstract

研究了双曲正割光束在分数衍射和矩形势竞争下的动力学。研究发现,光束在不同条件下可以表现出反射、隧道和干涉,形成束缚态、光晶格或流纹或孤子。在线性条件下,当电势较宽时,光束在较深电势和较小入射角时表现为全反射,而在较浅电势和较大入射角时则表现为反射和隧道。当电势较窄时,会产生不规则的干涉图案和束缚态。此外,初始啁啾会导致光束传播过程中出现侧叶。当两束双曲正割光束从电势内部或外部对称入射时,会在电势内部产生干涉晶格或干涉条纹,这与光束的莱维指数、初始啁啾和入射角度有关。在非线性状态下,双曲正割光束会通过选择适当的参数(包括莱维指数、初始奇异点和入射角)发生坍缩、分裂或形成周期样孤子。此外,还详细研究了两个双曲正割光束在非线性效应和分数衍射相互作用下的动态。这项工作为光学晶格生成和光学操纵提供了更多可能性。
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引用次数: 0
Controllable nonreciprocity based on a coupling-tunable waveguide 基于耦合可调波导的可控非互斥性
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-07-31 DOI: 10.1140/epjd/s10053-024-00898-4
Da-Liu Zheng, Jun-Fang Wu, Chao Li

Most of the previously proposed methods for nonreciprocal light transmission are based on the unequal couplings of the nanocavity with the input waveguide and the output waveguide, which will inevitably affect the contrast ratio and working bandwidth. Here, we present a simple approach just via the side coupling between one nonlinear resonator and a coupling-tunable waveguide, demonstrating that a high transmission contrast, broad operation bandwidth, and controllable nonreciprocal light transmission can be realized even though the coupling is symmetric. The underlying physics is revealed. This approach may open a way for the study of on-chip optical information processing and quantum computing.

Graphical abstract

Reconfigurable nonreciprocal light transmission with high contrast and broad operation bandwidth

之前提出的大多数非互易光传输方法都是基于纳米腔与输入波导和输出波导的不等耦合,这将不可避免地影响对比度和工作带宽。在这里,我们提出了一种仅通过一个非线性谐振器和一个耦合可调波导之间的侧耦合的简单方法,证明即使耦合是对称的,也能实现高传输对比度、宽工作带宽和可控的非互易光传输。揭示了其基本物理原理。这种方法可为片上光信息处理和量子计算的研究开辟道路。
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引用次数: 0
Differential elastic scattering and electron-impact ionization cross sections of nitrous oxide 一氧化二氮的差弹性散射和电子撞击电离截面
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-07-30 DOI: 10.1140/epjd/s10053-024-00880-0
M. Dinger, Y. Park, W. Y. Baek

With the aim of providing datasets for simulations of electron transport processes in the upper atmosphere, we measured singly differential elastic electron scattering and doubly differential electron-impact ionization cross sections of nitrous oxide. These measurements were conducted for primary electron energies between 30 eV and 1 keV in the angular range of 20°–150°. Secondary electron energies spanned from 4 eV to approximately half of the primary electron energy. In addition to the measurements, the differential elastic scattering cross sections of nitrous oxide were calculated using the IAM-SCAR + I model. Furthermore, the singly differential and total ionization cross sections of nitrous oxide were obtained by integrating the doubly differential ionization cross sections over emission angle and over both emission angle and secondary electron energy, respectively. These cross sections were compared to calculations performed using the BEB model and to experimental results of other groups, who determined the total ionization cross sections of nitrous oxide by collecting ions generated during electron impact.

Graphical abstract

为了给模拟高层大气电子传输过程提供数据集,我们测量了一氧化二氮的单差分弹性电子散射和双差分电子撞击电离截面。这些测量是在 20°-150° 角范围内对 30 eV 至 1 keV 的一次电子能量进行的。二次电子能量的范围从 4 eV 到一次电子能量的一半左右。除测量结果外,还利用 IAM-SCAR + I 模型计算了一氧化二氮的差分弹性散射截面。此外,通过对发射角的双差分电离截面以及发射角和二次电子能量的双差分电离截面进行积分,分别得到了一氧化二氮的单差分电离截面和总电离截面。这些截面与使用 BEB 模型进行的计算结果以及其他研究小组的实验结果进行了比较。
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引用次数: 0
High-resolution laboratory measurements of M-shell Fe EUV line emission using EBIT-I 利用 EBIT-I 高分辨率实验室测量 M 壳铁超紫外线发射
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-07-29 DOI: 10.1140/epjd/s10053-024-00891-x
Alexander J. Fairchild, Natalie Hell, Peter Beiersdorfer, Gregory V. Brown, Megan E. Eckart, Michael Hahn, Daniel W. Savin

Solar physicists routinely utilize observations of Ar-like Fe IX and Cl-like Fe X emission to study a variety of solar structures. However, unidentified lines exist in the Fe IX and Fe X spectra, greatly impeding the spectroscopic diagnostic potential of these ions. Here, we present measurements using the Lawrence Livermore National Laboratory EBIT-I electron beam ion trap in the wavelength range 238–258 Å. These studies enable us to unambiguously identify the charge state associated with each of the observed lines. This wavelength range is of particular interest because it contains the Fe IX density diagnostic line ratio 241.74 Å/244.91 Å, which is predicted to be one of the best density diagnostics of the solar corona, as well as the Fe X 257.26 Å magnetic-field-induced transition. We compare our measurements to the Fe IX and Fe X lines tabulated in CHIANTI v10.0.1, which is used for modeling the solar spectrum. In addition, we have measured previously unidentified Fe X lines that will need to be added to CHIANTI and other spectroscopic databases.

太阳物理学家通常利用对 Ar 类 Fe IX 和 Cl 类 Fe X 发射的观测来研究各种太阳结构。然而,Fe IX 和 Fe X 光谱中存在未识别线,极大地阻碍了这些离子的光谱诊断潜力。在此,我们介绍了使用劳伦斯-利弗莫尔国家实验室 EBIT-I 电子束离子阱在 238-258 Å 波长范围内进行的测量。我们对这一波长范围特别感兴趣,因为它包含了铁 IX 密度诊断线比率 241.74 Å/244.91 Å(据预测这是日冕的最佳密度诊断线之一),以及铁 X 257.26 Å 磁场诱导转变。我们将测量结果与用于太阳光谱建模的 CHIANTI v10.0.1 中列出的铁 IX 和铁 X 线进行了比较。此外,我们还测量了以前未识别的铁 X 线,这些线需要添加到 CHIANTI 和其他光谱数据库中。
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引用次数: 0
A two-state Kalman estimator for atomic gravimetry 用于原子重力测量的双态卡尔曼估计器
IF 1.5 4区 物理与天体物理 Q3 OPTICS Pub Date : 2024-07-24 DOI: 10.1140/epjd/s10053-024-00888-6
Bo-Nan Jiang

We present a two-state Kalman estimator of gravity acceleration and evaluate its performance by numerical simulations and post-measurement demonstration with real-world atomic gravimetry. We show that the estimator-enhanced gravimetry significantly improves upon both short-term sensitivity and long-term stability. The estimates of gravity acceleration demonstrate a (tau ^{1/2}) feature well under white phase noise in the short term, and continue to improve as (tau ^{-1/2}) or improve faster as (tau ^{-1}) in the long term. This work validates the estimation of gravity acceleration as a key topic for future atomic gravimetry.

The performance of atomic gravimetry is limited by noises and other systematic or geophysical effects. By building a Kaman estimator rooted in the physics of atom interferometry, we realize significant improvements in both short-term sensitivity and long-term stability. This demonstration of estimator-enhanced gravimetry would be of great interest for static measurements of gravity, such as metrology or geophysics (Color online)

摘要 我们提出了重力加速度的双状态卡尔曼估计器,并通过数值模拟和实际原子重力测量的测量后演示对其性能进行了评估。我们的研究表明,估计器增强的重力测量法显著提高了短期灵敏度和长期稳定性。重力加速度的估计值在短期内表现出了(tau ^{1/2})的特征,并且在长期内随着(tau ^{-1/2})的提高而继续提高,或者随着(tau ^{-1})的提高而更快地提高。这项工作验证了重力加速度的估计是未来原子重力测量的一个关键课题。通过建立植根于原子干涉测量物理学的卡曼估计器,我们实现了短期灵敏度和长期稳定性的显著提高。这种估算器增强重力测量法的演示对于重力的静态测量,如计量学或地球物理学,将具有极大的意义(彩色在线版)
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引用次数: 0
期刊
The European Physical Journal D
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