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Extraction evolutionary features of continuous light-induced plasmonic nanobubbles by a dynamic spectral regression model 利用动态光谱回归模型提取连续光诱导的等离子纳米气泡的演化特征
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-14 DOI: 10.1016/j.jqsrt.2024.109147
Yifan Zhang , Wei An , Yao Qin

A comprehensive understanding of the nature of light-induced plasmonic nanobubbles (PNBs) generated around noble metal nanoparticles is essential for optimizing PNB-based applications, such as light-driven microfluidic control. To investigate the overall evolution pattern of plasmonic nanobubbles (PNBs) under continuous light illumination, a computational model based on the least-squares method is established. Meanwhile, the variations in nanofluid transmittance and vaporization mass under continuous light illumination are measured by an immersion fiber and an electronic balance, respectively. The effects of nanoparticle concentration on the nanofluid transmittance and vaporization mass are analyzed. Considering the variations in nanofluid concentration, the overall evolution pattern of PNBs is preliminarily analyzed by monitoring the real-time dynamic change in nanofluid transmittance. The experimental results indicate that the nanoparticle concentration has an important effect on the nanofluid vaporization process. During the illumination stage, an increased nanofluid concentration intensifies the synergistic effect of water vaporization and PNB growth on transmittance reduction. The change in nanofluid transmittance caused by PNB scattering greatly exceeds that caused by increasing nanoparticle concentration. The nanofluid concentration gradually increases and peaks at the end of the cooling stage, and the rate of change of the nanofluid concentration is proportional to the nanofluid concentration. The numerical calculations show that the average size and the range of the PNB size distribution continuously increase with increasing irradiation time, and decrease during the cooling stage. A higher nanofluid concentration corresponds to a wider range of PNB size distribution.

全面了解贵金属纳米粒子周围产生的光诱导质子纳米气泡(PNB)的性质,对于优化基于 PNB 的应用(如光驱动微流体控制)至关重要。为了研究连续光照下等离子纳米气泡(PNBs)的整体演化模式,建立了一个基于最小二乘法的计算模型。同时,利用浸入式光纤和电子天平分别测量了连续光照下纳米流体透射率和汽化质量的变化。分析了纳米粒子浓度对纳米流体透射率和汽化质量的影响。考虑到纳米流体浓度的变化,通过监测纳米流体透过率的实时动态变化,初步分析了 PNB 的整体演化规律。实验结果表明,纳米粒子浓度对纳米流体气化过程有重要影响。在照明阶段,纳米流体浓度的增加会加强水汽化和 PNB 生长对透射率降低的协同效应。PNB 散射引起的纳米流体透射率变化大大超过纳米粒子浓度增加引起的变化。纳米流体浓度逐渐增加,并在冷却阶段结束时达到峰值,纳米流体浓度的变化率与纳米流体浓度成正比。数值计算表明,随着辐照时间的增加,PNB 的平均粒度和粒度分布范围不断增大,而在冷却阶段则不断减小。纳米流体浓度越高,PNB 尺寸分布范围越广。
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引用次数: 0
Mid-infrared high-resolution dual-comb spectroscopy: Intensity, broadening, and beyond-Voigt parameters of 12C2H2 and 13C12CH2 lines 中红外高分辨率双梳光谱:省略公式]和[省略公式]线的强度、展宽和超越-Voigt 参数
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-13 DOI: 10.1016/j.jqsrt.2024.109149
Nicolas Dricot, Bastien Vispoel, Muriel Lepère
<div><p>Using a high-resolution mid-infrared dual-comb spectrometer operating in the 1300 cm<sup>−1</sup> spectral region, spectra of acetylene were recorded at room temperature. Spectroscopic parameters were measured in 3 vibrational bands of both <span><math><mrow><msup><mrow></mrow><mrow><mn>12</mn></mrow></msup><msub><mrow><mtext>C</mtext></mrow><mrow><mn>2</mn></mrow></msub><msub><mrow><mtext>H</mtext></mrow><mrow><mn>2</mn></mrow></msub></mrow></math></span> and <span><math><mrow><msup><mrow></mrow><mrow><mn>13</mn></mrow></msup><msup><mrow><mtext>C</mtext></mrow><mrow><mn>12</mn></mrow></msup><msub><mrow><mtext>CH</mtext></mrow><mrow><mn>2</mn></mrow></msub></mrow></math></span>. Absolute line intensities (<span><math><msub><mrow><mi>S</mi></mrow><mrow><mn>0</mn></mrow></msub></math></span>) and self-broadening coefficients (<span><math><msubsup><mrow><mi>γ</mi></mrow><mrow><mn>0</mn></mrow><mrow><mi>s</mi><mi>e</mi><mi>l</mi><mi>f</mi></mrow></msubsup></math></span>) were determined in the <span><math><mrow><msub><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ν</mi></mrow><mrow><mn>5</mn></mrow></msub></mrow></math></span>, <span><math><mrow><mn>2</mn><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>2</mn></mrow></msubsup><mo>+</mo><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>5</mn></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msubsup><mover><mrow><mo>⟵</mo></mrow><mrow></mrow></mover><mspace></mspace><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>1</mn></mrow></msubsup></mrow></math></span> and <span><math><mrow><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow><mrow><mn>1</mn></mrow></msubsup><mo>+</mo><mn>2</mn><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>5</mn></mrow><mrow><mn>0</mn></mrow></msubsup><mover><mrow><mo>⟵</mo></mrow><mrow></mrow></mover><mspace></mspace><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>5</mn></mrow><mrow><mn>1</mn></mrow></msubsup></mrow></math></span> bands. For the main isotopologue, the collisional narrowing coefficients (<span><math><msubsup><mrow><mi>ν</mi></mrow><mrow><mn>0</mn></mrow><mrow><mi>V</mi><mi>C</mi></mrow></msubsup></math></span>) as well as the speed-dependence of the broadening (<span><math><msub><mrow><mi>γ</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>) and shifting (<span><math><msub><mrow><mi>δ</mi></mrow><mrow><mn>2</mn></mrow></msub></math></span>) coefficients were measured in the <span><math><mrow><msub><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ν</mi></mrow><mrow><mn>5</mn></mrow></msub></mrow></math></span> band of the main isotopologue of acetylene. Theoretical line-shape models were fitted on experimental profiles using a homemade multi-spectrum fitting procedure to determine spectroscopic parameters. Excellent agreement with the literature was found for self-broadening coefficients and absolute line intensities in the <span><math><mrow><msub><mrow><mi>ν</mi></mrow><mrow><mn>4<
利用在 1300 厘米光谱区工作的高分辨率中红外双梳光谱仪,在室温下记录了乙炔的光谱。测量了乙炔和乙炔的 3 个振动波段的光谱参数。测定了 、 和 波段的绝对线强度()和自扩系数()。在乙炔主要同素异形体的波段中,测量了碰撞收窄系数()以及增宽()和移动()系数的速度依赖性。使用自制的多光谱拟合程序将理论线形模型拟合到实验剖面上,以确定光谱参数。在乙炔波段的自扩频系数和绝对线强度方面,发现与文献有很好的一致性。 在热波段方面,发现在实验不确定性范围内与文献有很好的一致性,而这些热波段也是首次报道。同样,发现的旋转依赖性与以前的研究结果接近。
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Spectroscopic parameters were measured in 3 vibrational bands of both &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mtext&gt;C&lt;/mtext&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mtext&gt;H&lt;/mtext&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;13&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mtext&gt;C&lt;/mtext&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mtext&gt;CH&lt;/mtext&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;. Absolute line intensities (&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;) and self-broadening coefficients (&lt;span&gt;&lt;math&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;γ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;s&lt;/mi&gt;&lt;mi&gt;e&lt;/mi&gt;&lt;mi&gt;l&lt;/mi&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;) were determined in the &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mover&gt;&lt;mrow&gt;&lt;mo&gt;⟵&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;/mover&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;mover&gt;&lt;mrow&gt;&lt;mo&gt;⟵&lt;/mo&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;/mover&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; bands. For the main isotopologue, the collisional narrowing coefficients (&lt;span&gt;&lt;math&gt;&lt;msubsup&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/msubsup&gt;&lt;/math&gt;&lt;/span&gt;) as well as the speed-dependence of the broadening (&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;γ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;) and shifting (&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;δ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;) coefficients were measured in the &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; band of the main isotopologue of acetylene. Theoretical line-shape models were fitted on experimental profiles using a homemade multi-spectrum fitting procedure to determine spectroscopic parameters. Excellent agreement with the literature was found for self-broadening coefficients and absolute line intensities in the &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;","PeriodicalId":16935,"journal":{"name":"Journal of Quantitative Spectroscopy & Radiative Transfer","volume":"328 ","pages":"Article 109149"},"PeriodicalIF":2.3,"publicationDate":"2024-08-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142043731","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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
High-accuracy optical clocks with sensitivity to the fine-structure constant variation based on Sm10+ 基于 Sm10+ 的对精细结构常数变化敏感的高精度光学时钟
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-13 DOI: 10.1016/j.jqsrt.2024.109151
Saleh O. Allehabi , V.A. Dzuba , V.V. Flambaum

We identify two metastable excited states in Sm10+ highly charged ion as candidates for high accuracy optical clocks. Several atomic properties relevant to optical clock development are calculated using relativistic many-body methods. This includes energy levels, transition amplitudes, lifetimes, scalar polarizabilities, black body radiation shift, and the sensitivity to the fine structure constant variation. We found that the clock transitions are not sensitive to perturbation, e.g., relative black body radiation shifts are 1019. The enhancement factor for the α variation is 0.8 for one clock transition and 16 for another.

我们确定了 Sm10+ 高电荷离子中的两个瞬变激发态作为高精度光学钟的候选态。我们使用相对论多体方法计算了与光学时钟开发相关的几个原子特性。其中包括能级、跃迁振幅、寿命、标量极化率、黑体辐射位移以及对精细结构常数变化的敏感性。我们发现时钟跃迁对扰动并不敏感,例如,相对黑体辐射位移为 10-19 ∼ 10-19。一个时钟转换的α变化增强因子为0.8,另一个时钟转换的α变化增强因子为16。
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引用次数: 0
Temperature dependence of line shape parameters for N2- and O2-broadened methane lines by quantum cascade laser spectroscopy 量子级联激光光谱法测量 N2- 和 O2 扩宽甲烷线的线形参数与温度的关系
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-13 DOI: 10.1016/j.jqsrt.2024.109150
B. Vispoel, T. Roland, O. Browet, M. Lepère

This paper report nitrogen- and oxygen-broadening coefficients, their speed-dependencies, and the collisional narrowing parameters of lines in the ν4-band of methane. The parameters were determined from low (150 K) to high temperatures (600 K). The measurements were done with a high-resolution quantum cascade laser spectrometer coupled to specific absorption cells that allow to cool and heat the gas mixtures with a great stability. The spectroscopic parameters were determined at each temperature by fits of the experimental absorbances in a multispectrum fitting procedure using the Voigt, Speed-Dependent Voigt, Nelkin-Ghatak and Speed-dependent Nelkin-Ghatak theoretical line shape models. The temperature dependencies of the collisional half-widths, the speed-dependence of the broadening coefficients as well as the collisional narrowing parameters were studied with the empirical power law and the physics-based Gamache-Vispoel model (DPL) [Gamache and Vispoel, JQSRT, 217, 440–452, 2018]. The obtained line shape parameters and their temperature dependencies are compared, when possible, to existing data in literature. The DPL reproduces more accurately the evolution of the studied collisional parameters over the wide range of temperature considered in the study.

本文报告了甲烷 ν4 波段中的氮和氧展宽系数、其速度依赖性以及碰撞窄化参数。这些参数是从低温(150 K)到高温(600 K)测定的。测量是通过高分辨率量子级联激光光谱仪与特定吸收池耦合完成的,该吸收池可以非常稳定地冷却和加热混合气体。在每个温度下的光谱参数都是通过使用 Voigt、依赖速度的 Voigt、Nelkin-Ghatak 和依赖速度的 Nelkin-Ghatak 理论线形模型对实验吸光度进行多光谱拟合而确定的。利用经验幂律和基于物理学的 Gamache-Vispoel 模型(DPL)[Gamache 和 Vispoel,JQSRT,217,440-452,2018]研究了碰撞半宽的温度依赖性、增宽系数的速度依赖性以及碰撞收窄参数。在可能的情况下,将获得的线形参数及其温度依赖性与文献中的现有数据进行比较。DPL 更准确地再现了研究中考虑的宽温度范围内所研究的碰撞参数的演变。
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引用次数: 0
The ammonia absorption spectrum between 3900 and 6350 cm-1: 15NH3 contribution and a recommended list for natural ammonia 3900 和 6350 cm-1 之间的氨吸收光谱:15NH3 的贡献和天然氨的建议清单
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-10 DOI: 10.1016/j.jqsrt.2024.109148
P. Cacciani , P. Čermák , J. Vander Auwera , A. Campargue

Following previous contributions dedicated to the main isotopologue, 14NH3, in the present work, we examine the 15NH3 absorption spectrum between 3950 and 6350 cm-1 in order to elaborate an absorption line list for ammonia in natural isotopic abundance. For this purpose, several room temperature Fourier Transform absorption spectra of ammonia highly enriched in 15NH3 measured in the 90′s and available from the Kitt Peak data centre have been analysed. In addition, a more recent high-resolution spectrum recorded in Brussels between 4150 and 4600 cm-1 is also considered. The spectra were divided in three separate intervals (3900–4706, 4706–5650 and 5650–6350 cm-1) for which experimental lists including 3506, 3788, and 2317 lines, respectively, were retrieved and treated independently. By comparison with an ab initio line list (the BYTe list) and systematically validating the assignments by using lower state combination difference relations (LSCD), 2013, 1771 and 570 transitions could be assigned in the three regions, respectively. They belong to 16, 22, and 10 bands and correspond to 98.5, 92.6 and 78.6 % of the experimental intensities in the region, respectively. For comparison, only four 15NH3 bands were previously assigned in the literature in the entire studied region.

The obtained 15NH3 assigned line lists were gathered with the previously elaborated line list of the main isotopologue to produce a recommended line list for natural ammonia between 3900 and 6350 cm-1.

继之前对主要同素异形体 14NH3 的研究之后,在本研究中,我们研究了 3950 和 6350 cm-1 之间的 15NH3 吸收光谱,以便为天然同位素丰度的氨制定一个吸收线表。为此,我们分析了基特峰数据中心在 90 年代测量到的 15NH3 高浓度氨的室温傅立叶变换吸收光谱。此外,还考虑了在布鲁塞尔记录的 4150 至 4600 cm-1 之间的最新高分辨率光谱。光谱被分为三个独立的区间(3900-4706、4706-5650 和 5650-6350cm-1),分别检索并独立处理了包括 3506、3788 和 2317 条谱线在内的实验清单。通过与 ab initio 线表(BYTe 表)进行比较,并利用低态组合差分关系(LSCD)对分配进行系统验证,可以在这三个区域分别分配到 2013、1771 和 570 个跃迁。它们分别属于 16、22 和 10 个波段,分别相当于该区域实验强度的 98.5%、92.6% 和 78.6%。将所获得的 15NH3 谱线表与先前制定的主要同素异形体谱线表汇集在一起,得出了 3900 至 6350 cm-1 之间天然氨的推荐谱线表。
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引用次数: 0
Research on the modeling technique of infrared radiation scaling law for rocket engine exhaust plumes 火箭发动机排气烟羽红外辐射缩放规律建模技术研究
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-05 DOI: 10.1016/j.jqsrt.2024.109146
Yiqiang Sun , Qinglin Niu , Tanxiao Zhu , Guanglu Zhang , Zhihong He , Shikui Dong

The complexity of the rocket motor exhaust plume radiation phenomenon, along with the influence of numerous parameters and implicit propagation, makes the theoretical simulation calculations expensive. This hinders design optimization, parameter identification, and other studies. Hence, it is crucial to establish the direct correlation between thrust, velocity, altitude, detection angle, and plume radiation in engineering.

The paper proposes a scaling law modeling approach for predicting plume infrared radiation from liquid oxygen (LOX)/kerosene rocket engines to solve the difficulties of quick prediction and lack of explicit models. An explicit scaling law model with four parameters is developed by utilizing the e-exponential scaling law to relate plume radiance to flight velocity, the power scaling law to relate plume radiance to vacuum thrust, and the sinusoidal scaling law to relate plume radiance to detection angle. This model employs a decoupled modeling approach for plume radiance, flight altitude, flight velocity, vacuum thrust, and detection angle. A fast prediction method for the LOX/kerosene rocket engine plume in the altitude range of 11∼61 km is achieved. The theoretical simulation test shows the relative error of the velocity-scaling law in predicting the radiance of the RD-180 template engine during the Atlas III flight trajectory is less than 20 %. The radiance of the RD-170 and RD-191 rocket engines is predicted using the thrust-scaling law based on the radiance of the RD-180 template engine exhaust plume. The radiance of the exhaust plume from the RD-170 and RD-191 rocket motors is estimated using the thrust-scaling law with an accuracy of under 15 %. Subsequently, the radiance of these two motors at detection angles between 10° and 170° is predicted using the angle-scaling with a relative error of less than 35 %.

火箭发动机排气烟羽辐射现象复杂,受众多参数和隐式传播的影响,使得理论模拟计算费用昂贵。这阻碍了设计优化、参数识别和其他研究。因此,在工程中建立推力、速度、高度、探测角和烟羽辐射之间的直接相关性至关重要。本文提出了一种预测液氧(LOX)/煤油火箭发动机烟羽红外辐射的缩放定律建模方法,以解决快速预测和缺乏显式模型的难题。通过利用电子指数缩放定律将烟羽辐射率与飞行速度联系起来,利用功率缩放定律将烟羽辐射率与真空推力联系起来,以及利用正弦缩放定律将烟羽辐射率与探测角联系起来,建立了一个具有四个参数的显式缩放定律模型。该模型对羽流辐射度、飞行高度、飞行速度、真空推力和探测角采用了解耦建模方法。实现了对 11~61 km 高度范围内的 LOX/ 煤油火箭发动机烟羽的快速预测。理论模拟测试表明,速度缩放定律在预测 Atlas III 飞行轨迹中 RD-180 模板发动机辐射度时的相对误差小于 20%。RD-170和RD-191火箭发动机的辐射率是根据RD-180模板发动机排气烟羽的辐射率使用推力缩放定律预测的。RD-170 和 RD-191 火箭发动机废气烟羽的辐射度是根据推力缩放定律估算的,精度低于 15%。随后,利用角度缩放法预测了这两台发动机在 10° 至 170° 检测角上的辐射率,相对误差小于 35%。
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引用次数: 0
2D Raman imaging for vibrational and rotational temperature mapping in H2 二维拉曼成像绘制 H2 的振动和旋转温度图
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-08-05 DOI: 10.1016/j.jqsrt.2024.109145
D. Del Cont-Bernard, M.D. Ruijzendaal, T.W.H. Righart, G.J. van Rooij, T.D. Butterworth

We showcase a Raman scattering diagnostic for 2D imaging of the rotational and vibrational temperatures of H2. Applications include environments with vibrational-rotational non-equilibrium such as H2-containing supersonic jets and plasma reactors. We image segments of the laser scattering spectrum, containing one or more Raman features, using an ICCD camera that is equipped with one of several bandpass filters. Knowing their transmission spectrum allows the construction of calibration curves that relate the relative intensities of the multi-spectral image to the rotational and vibrational temperatures. Additionally, the absolute intensity indicates the density of H2. We illustrate the capability to independently measure rotational (300–3000 K, ±150 K) and vibrational temperatures (1000–3000 K, ±50 K). The technique is demonstrated on two different H2 microwave plasmas and validated against conventional fitting of 0D and 1D Raman spectra.

我们展示了一种用于 H2 旋转和振动温度二维成像的拉曼散射诊断方法。其应用包括振动-旋转非平衡环境,如含 H2 的超音速喷流和等离子反应堆。我们使用装有多个带通滤波器的 ICCD 相机对包含一个或多个拉曼特征的激光散射光谱片段进行成像。通过了解其透射光谱,可以构建校准曲线,将多光谱图像的相对强度与旋转和振动温度联系起来。此外,绝对强度还能显示 H2 的密度。我们展示了独立测量旋转温度(300-3000 K,±150 K)和振动温度(1000-3000 K,±50 K)的能力。该技术在两个不同的 H2 微波等离子体上进行了演示,并与传统的 0D 和 1D 拉曼光谱拟合进行了验证。
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引用次数: 0
Analysis of the extreme ultraviolet broadband spectral characteristics and spatiotemporal evolution of laser-produced germanium plasmas 激光产生的锗等离子体的极紫外宽带光谱特性和时空演变分析
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-07-26 DOI: 10.1016/j.jqsrt.2024.109133
Yanhong Wu , Qi Min , Siqi He , Haidong Lu , Xingbang Liu , Kede Yang , Shiquan Cao , Duixiong Sun , Maogen Su , Chenzhong Dong

This paper presents comprehensive spectral measurements and a theoretical analysis of laser-produced germanium (Ge) plasma within the 7.5–17 nm wavelength range, with the measurements being performed using spatiotemporally-resolved emission spectroscopy. We obtained and analyzed the extreme ultraviolet (EUV) spectra and their variations meticulously at various positions adjacent to the target surface. The 3p and 3d excitations of Ge ions spanning from Ge4+ to Ge13+ were calculated using the Cowan configuration interaction codes, with particular emphasis being placed on analysis of the spectral line distributions in the 3d-np, 3d-nf, and 3p-3d, 4s, 4d transition arrays. This analysis indicated the contributions made by these transition arrays to the broadband spectral features that were observed experimentally. By using a steady-state collisional radiation model along with a normalized Boltzmann distribution assumption, we clarified the predominant contributions of the 3d-4p and 3p-3d transitions from the Ge7+ to Ge9+ ions in close proximity to the target surface, along with those from the Ge5+ and Ge6+ ions at greater distances. Furthermore, by combining the results above with a plasma dynamics evolution analysis, we gained insights into how the plasma's transient and nonuniform properties influence the analysis of complex EUV band spectral profiles and examine their implications for spectral diagnostics. These results will be useful for plasma spectral diagnosis and for application to development of pulsed short-wavelength light sources.

本文介绍了 7.5-17 纳米波长范围内激光产生的锗(Ge)等离子体的全面光谱测量和理论分析,测量采用时空分辨发射光谱法进行。我们获得并分析了极紫外(EUV)光谱及其在目标表面附近不同位置的变化。我们使用 Cowan 配置相互作用代码计算了从 Ge4+ 到 Ge13+ 的 Ge 离子的 3p 和 3d 激发,重点分析了 3d-np、3d-nf 和 3p-3d、4s、4d 过渡阵列的光谱线分布。该分析表明了这些转变阵列对实验观察到的宽带光谱特征的贡献。通过使用稳态碰撞辐射模型和归一化玻尔兹曼分布假设,我们明确了来自靠近靶表面的 Ge7+ 至 Ge9+ 离子的 3d-4p 和 3p-3d 转变,以及来自较远距离的 Ge5+ 和 Ge6+ 离子的转变的主要贡献。此外,通过将上述结果与等离子体动力学演化分析相结合,我们深入了解了等离子体的瞬态和非均匀特性如何影响复杂超紫外波段光谱剖面的分析,并研究了它们对光谱诊断的影响。这些结果将有助于等离子体光谱诊断和脉冲短波长光源的开发。
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引用次数: 0
Spectro-polarimetric backscattering of atmospheric particles 大气颗粒的光谱-偏振后向散射
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-07-25 DOI: 10.1016/j.jqsrt.2024.109132
Killian Aleau , Romain Ceolato , Matthew Berg , Guillaume Huss , Olga Muñoz , Gorden Videen

This study presents a new experiment to measure the polarization-resolved two-dimensional light-scattering patterns, near and including the backscattering direction, of fixed particles representative of some atmospheric-aerosol types. The measurements are conducted across a broad spectrum, from 450 to 850 nm, and for different polarization states. A supercontinuum laser, achromatic optics, and polarizers are used to measure the scattering patterns. Important quantities for applications such as lidar are also measured including the backscattering phase-function and the linear depolarization ratio in the exact backscattering direction. Microscopic images of the particles are provided by digital in-line holography as well. Thus, in some cases, it is possible to interpret the spectro-polarimetric measurements with knowledge of the size and shape of the particles involved. Spherical particles of known properties are used to calibrate the method. Then, Arizona test dust, Gobi and Sahara Desert dust, and ash from the Eyjafjallajökull and La Palma volcanic eruptions are studied to illustrate the method's potential for lidar applications.

本研究介绍了一种新的实验,用于测量代表某些大气气溶胶类型的固定颗粒的偏振分辨二维光散射图样,包括反向散射方向附近的散射图样。测量的光谱范围很广,从 450 纳米到 850 纳米,并针对不同的偏振态。测量散射模式时使用了超连续激光器、消色差光学器件和偏振器。此外,还测量了激光雷达等应用的重要数据,包括精确反向散射方向上的反向散射相位函数和线性去极化率。数字在线全息技术还能提供颗粒的微观图像。因此,在某些情况下,可以通过了解相关颗粒的尺寸和形状来解释光谱极化测量结果。已知性质的球形颗粒用于校准该方法。然后,研究了亚利桑那测试尘埃、戈壁和撒哈拉沙漠尘埃以及埃亚菲亚德拉角火山和拉帕尔马火山喷发的火山灰,以说明该方法在激光雷达应用方面的潜力。
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引用次数: 0
CaSDa24: Latest updates to the Dijon calculated spectroscopic databases CaSDa24:第戎计算光谱数据库的最新更新
IF 2.3 3区 物理与天体物理 Q2 OPTICS Pub Date : 2024-07-23 DOI: 10.1016/j.jqsrt.2024.109127
C. Richard , O. Ben Fathallah , P. Hardy , R. Kamel , M. Merkulova , M. Rotger , O.N. Ulenikov , V. Boudon

We introduce CaSDa24, the latest iteration of our high-resolution molecular spectroscopy database cluster. Comprising ten independent databases, each dedicated to a specific molecule (CH4, CH3Cl, SF6, C2H4, CF4, GeH4, RuO4, SiF4, UF6, SiH4), CaSDa24 integrates updated and new databases since our previous publication. These databases include detailed lists of calculated spectral lines, eigenvectors, energy levels, and additional relevant information derived from the latest experimental spectra analyses. This article provides an overview of the current state of molecular spectroscopy databases, explains the foundational principles of CaSDa24, and summarizes the significant updates and new data introduced.

我们介绍的是高分辨率分子光谱数据库集群的最新迭代。该数据库集群由十个独立的数据库组成,每个数据库专门针对一种特定的分子(CH、CHCl、SF、CH、CF、GeH、RuO、SiF、UF、SiH)。这些数据库包括计算光谱线、特征向量、能级的详细列表,以及从最新实验光谱分析中获得的其他相关信息。这篇文章概述了分子光谱数据库的现状,解释了分子光谱数据库的基本原理,并总结了引入的重要更新和新数据。
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引用次数: 0
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Journal of Quantitative Spectroscopy & Radiative Transfer
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