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Emulating non-gray gas radiative heat transfer in combustion scenarios by machine learning method 利用机器学习方法模拟燃烧工况下非灰色气体的辐射传热
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-11-04 DOI: 10.1016/j.jqsrt.2025.109735
Yujia Sun , Chenxin Lin , Shu Zheng
Thermal radiation plays an important role in combustion systems due to its significant effect on the energy evolution. Radiation modeling in combustion simulations needs expensive computational resources due to high complexity of the radiative transfer equation and highly variations of the spectral radiative properties. Traditional numerical methods for the radiation modeling have many simplified and approximated models, but they are still suffering from the irreconcilable conflict between the accuracy and efficiency. This work investigates the capability of machine learning for predicting radiative heat transfer in combustion scenarios. Two machine learning models, UNet model and Fourier network operator (FNO) model are designed to learn radiative heat transfer directly from the temperature and concentrations fields. Their performances are tested for a turbulent diffusion flame. Results show that both UNet and FNO performs well for emulating the radiative heat source for the considered flame, with relative errors generally smaller than 0.3 %. The two models have similar accuracies. This study demonstrates the feasibility of using UNet and FNO models as surrogate model for non-gray gas radiative heat transfer in combustion system, but they need further investigations for more complex combustion scenarios.
热辐射对燃烧系统的能量演化有重要影响,在燃烧系统中起着重要作用。燃烧模拟中的辐射建模由于辐射传递方程的高度复杂性和光谱辐射特性的高度变异性,需要耗费大量的计算资源。传统的辐射数值模拟方法有许多简化和近似的模型,但仍然存在精度和效率之间不可调和的冲突。这项工作研究了机器学习预测燃烧场景中辐射传热的能力。设计了两个机器学习模型,UNet模型和傅立叶网络算子(FNO)模型,直接从温度和浓度场中学习辐射传热。在紊流扩散火焰中测试了它们的性能。结果表明,UNet和FNO都能很好地模拟所考虑火焰的辐射热源,相对误差一般小于0.3%。这两种模型具有相似的精度。本研究证明了使用UNet和FNO模型作为燃烧系统非灰气体辐射换热的替代模型的可行性,但需要对更复杂的燃烧场景进行进一步的研究。
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引用次数: 0
O2- and air-broadening coefficients in the ν2 and ν5 bands of CH3Br CH3Br ν2和ν5波段的O2-和空气展宽系数
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-11-01 DOI: 10.1016/j.jqsrt.2025.109723
I. Majdi , S. Harbaoui , D. Ben Abdallah , J. Salem , Z. Boussetta , F. Kwabia Tchana , X. Landsheere , A. Voute , M. Hochlaf , H. Aroui
In the present work, we measured the O2-broadening coefficients of the absorption lines in the ν2 and ν5 bands of methyl bromide at room temperature (T = 295 K) using a high-resolution Fourier Transform spectrometer. Eight spectra were recorded at pressures ranging from 2.0 to 6.5 Torr for the active gas and from 3 to 90 Torr for the perturber gas. The line shape parameters were obtained by fitting Voigt and Galatry profiles to the measured line shapes, allowing the determination of the O2-broadening coefficients for the branches over the 1250 – 1622 cm-1 wavenumbers range. This range covers 1451 measured transitions with 2 ≤ J ≤ 54 and 0 ≤ K ≤ 10. These data, combined with previously measured N2-broadening coefficients, were used to determine the air-broadening coefficients of the ν2 and ν5 bands. Finally, an empirical model was used to fit the broadening coefficients of the two bands. On average, the empirical expression reproduces successfully the measured broadening coefficients.
本文用高分辨率傅立叶变换光谱仪测量了室温(T = 295 K)下甲基溴ν2和ν5波段吸收谱线的o2展宽系数。活性气体在2.0 ~ 6.5托的压力下,摄动气体在3 ~ 90托的压力下,记录了8个光谱。通过将Voigt和galry剖面拟合到测量的线形上,获得了线形参数,从而确定了分支在1250 - 1622 cm-1波数范围内的o2展宽系数。该范围涵盖了1451个2≤J≤54和0≤K≤10的测量跃迁。这些数据与先前测量的n2展宽系数相结合,用于确定ν2和ν5波段的空气展宽系数。最后,利用经验模型对两波段的展宽系数进行拟合。平均而言,经验表达式成功地再现了测量的展宽系数。
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引用次数: 0
Implementation of low stream interpolation technique to accelerate scattering calculations in the 4A/OP radiative transfer model 在4A/OP辐射传输模型中实现低流插值技术以加速散射计算
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-11-01 DOI: 10.1016/j.jqsrt.2025.109734
Bojan Sic , Elsa Jacquette , Denis Jouglet , Pierre Lafrique , Clemence Pierangelo , Raymond Armante , Olivier Lezeaux , Mahmoud El Hajj
Considering scattering in radiative transfer calculations often leads to extensively long computation times that can be prohibitive, especially in the operational context of satellite missions. Over time, numerous methods were developed to accelerate scattering calculations. In this paper, based and further built upon the work of O’Dell [1], we describe the implementation of the Low-Stream Interpolation acceleration technique in the 4A/OP radiative transfer model. The method’s acceleration relies on the execution of computationally expensive calculations only for representative points, which represent the regions in the gas absorption optical depth space called “bins”. For all other points the calculation is performed at a low accuracy and by subsequent interpolation. We have considered a number of method’s aspects, and introduced various modifications in order to optimise its accuracy and computation time. This includes: a) an extension of the method to Jacobians, b) modifications of bin and sub-bin divisions, c) implementation of automatic binning and its comparison to fixed bins, d) improvement of the computation of representative points, e) improvement of the definition of “significant scattering” used by the method, f) avoiding the redundancy of high-accuracy computation at large gas absorption optical depths, g) optimisations of the method computation domain size and h) evaluations of various possible accelerations of low-accuracy calculations. We applied the method on the MicroCarb O2 and CO2 bands in near-infrared and shortwave-infrared over a large variety of geophysical cases and discussed the impacts of the modifications and the overall performance. We confirmed that the Low-Stream Interpolation is a powerful technique to accelerate the scattering calculations and, in our model, it provided relative accuracies on polarised and unpolarised radiances and Jacobians lower than 0.05 % with acceleration of 10–50 times.
在辐射传输计算中考虑散射通常会导致计算时间过长,这可能令人望而却步,特别是在卫星任务的业务范围内。随着时间的推移,发展了许多方法来加速散射计算。本文在O 'Dell[1]的基础上,描述了低流插值加速技术在4A/OP辐射传输模型中的实现。该方法的加速依赖于只对代表性点执行计算昂贵的计算,这些代表性点代表气体吸收光学深度空间中的区域,称为“箱”。对于所有其他点,计算是在低精度和随后的插值执行。我们考虑了许多方法的方面,并引入了各种修改,以优化其精度和计算时间。这包括:a)将该方法推广到雅可比矩阵,b)修改本箱和子箱的划分,c)实现自动分箱及其与固定分箱的比较,d)改进代表性点的计算,e)改进该方法使用的“显著散射”的定义,f)避免在大气体吸收光学深度下高精度计算的冗余。G)方法计算域大小的优化和h)低精度计算的各种可能加速的评估。我们将该方法应用于近红外和短波红外的MicroCarb O2和CO2波段,并讨论了修改后的影响和整体性能。我们证实了低流插值是一种加速散射计算的强大技术,在我们的模型中,它提供了极化和非极化辐射和雅可比比的相对精度低于0.05%,加速度为10-50倍。
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引用次数: 0
Quality control for infrared radiance of geostationary meteorological satellite using imaginary signal of Fourier transform spectroscopy 利用傅里叶变换光谱虚信号控制地球同步气象卫星红外辐射质量
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-11-01 DOI: 10.1016/j.jqsrt.2025.109733
Yoshifumi Ota
In this study, we explored the spectral characteristics of radiance data collected by the Geostationary Interferometric Infrared Sounder (GIIRS) aboard the Feng-Yun-4B (FY-4B) geostationary meteorological satellite. We compared GIIRS brightness temperature observations with the first guess from the regional numerical weather forecast model of the Japan Meteorological Agency, and analyzed the bias errors in brightness temperature under clear-sky conditions. In the longwave band, we observed checkerboard patterns of bias error distributions in the CO2 channel. Focusing on the imaginary signals from the radiance data obtained through interferometry with a Fourier transform spectrometer, we believe that the observed bias errors are primarily attributed to electrical factors rather than GIIRS interferometry itself, and most of these errors can be corrected by estimating them in advance. Conversely, in the midwave band, we observed concave bias error distributions in the GIIRS instrument’s dwell, indicating that these may be related to GIIRS interferometry. Additionally, we examined the characteristics of the imaginary signal under cloudy conditions by comparing it with the cloud physical property products from Himawari-9. It was observed that large imaginary signals tended to appear in GIIRS data for scenes with high clouds and low brightness temperatures. This indicates that the imaginary signal could serve as auxiliary information for assessing whether observations are influenced by clouds, particularly high clouds including optically thin cirrus clouds. For the quantitative use of GIIRS data, it is important to consider these bias errors and perform quality control using the imaginary signal.
本文研究了风云- 4b (FY-4B)同步气象卫星上的地球同步干涉红外测深仪(GIIRS)采集的辐射数据的光谱特征。将GIIRS的亮度温度观测值与日本气象厅区域数值天气预报模式的首次估算值进行比较,分析了晴空条件下亮度温度的偏差。在长波波段,我们观察到CO2通道中的偏差误差分布呈棋盘状。通过傅里叶变换光谱仪干涉测量得到的辐射亮度数据中的虚信号,我们认为观测到的偏置误差主要是由电因素引起的,而不是由干涉测量本身引起的,这些误差大部分可以通过预先估计来纠正。相反,在中波波段,我们观察到GIIRS仪器驻留的凹偏置误差分布,表明这些可能与GIIRS干涉测量有关。此外,通过与Himawari-9的云物性产品进行比较,我们研究了多云条件下虚信号的特征。研究发现,在高云和低亮温的场景下,红外遥感数据往往出现较大的虚信号。这表明虚信号可以作为辅助信息,用于评估观测是否受到云的影响,特别是包括光学薄卷云在内的高空云。对于GIIRS数据的定量使用,重要的是要考虑这些偏差误差,并使用虚信号进行质量控制。
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引用次数: 0
High-resolution ro-vibrational analysis of HCFC-22: Deciphering ν4 and 2ν6 bands of 12CH35ClF2 and ν4 band of 13CH35ClF2 species HCFC-22的高分辨率反振动分析:破译12CH35ClF2的ν 4和2 ν 6波段和13CH35ClF2的ν 4波段
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-10-31 DOI: 10.1016/j.jqsrt.2025.109721
Egor O. Dobrolyubov , Ilya M. Efremov , Sergey V. Krasnoshchekov , Igor V. Polyakov , Vladimir B. Laptev , Sergey A. Klimin , Dmitry V. Millionshchikov , Olga V. Naumenko
<div><div>A ro-vibrational analysis of a high-resolution IR spectrum of an isotopic mixture of the atmospheric pollutant chlorodifluoromethane (HCFC-22), enriched in <sup>13</sup>C to 29.8 ± 0.14%, was performed in the range of 779–849 cm<sup>−1</sup>, and the identification of spectral features was limited to most abundant species <sup>12</sup>CH<sup>35</sup>ClF2 and <sup>13</sup>CH<sup>35</sup>ClF<sub>2</sub>. The spectrum was recorded on a Bruker IFS-125HR FT spectrometer at room temperature with a resolution of <span><math><mo>≈</mo></math></span>0.001 cm<sup>−1</sup>. The inverse spectroscopic problem for the main isotopologue <sup>12</sup>CH<sup>35</sup>ClF<sub>2</sub> was solved with Watson-type <span><math><mi>A</mi></math></span>-reduced effective Hamiltonian (<span><math><msub><mrow><mi>H</mi></mrow><mrow><mi>eff</mi></mrow></msub></math></span>) with accounting of the <span><math><mrow><msub><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow></msub><mo>/</mo><mn>2</mn><msub><mrow><mi>ν</mi></mrow><mrow><mn>6</mn></mrow></msub></mrow></math></span> Fermi resonance and 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>6</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ν</mi></mrow><mrow><mn>9</mn></mrow></msub></mrow></math></span> Coriolis resonance. The identified 3003 transitions of <span><math><msub><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow></msub></math></span> and 1265 transitions of <span><math><mrow><mn>2</mn><msub><mrow><mi>ν</mi></mrow><mrow><mn>6</mn></mrow></msub></mrow></math></span> produced 1598 empirical upper energy levels of the <span><math><msub><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow></msub></math></span> (<span><math><mrow><mi>J</mi><mo>≤</mo><mn>81</mn><mo>,</mo><msub><mrow><mi>K</mi></mrow><mrow><mi>a</mi></mrow></msub><mo>≤</mo><mn>13</mn></mrow></math></span>) and 840 levels of the <span><math><mrow><mn>2</mn><msub><mrow><mi>ν</mi></mrow><mrow><mn>6</mn></mrow></msub></mrow></math></span> band (<span><math><mrow><mi>J</mi><mo>≤</mo><mn>71</mn><mo>,</mo><msub><mrow><mi>K</mi></mrow><mrow><mi>a</mi></mrow></msub><mo>≤</mo><mn>11</mn></mrow></math></span>) with RMSD = 2.92<span><math><mrow><mo>×</mo><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>4</mn></mrow></msup></mrow></math></span> cm<sup>−1</sup>. For the <sup>13</sup>CH<sup>35</sup>ClF<sub>2</sub> isotopologue, 670 transitions and corresponding empirical 350 energy levels of <span><math><msub><mrow><mi>ν</mi></mrow><mrow><mn>4</mn></mrow></msub></math></span> band (<span><math><mrow><mi>J</mi><mo>≤</mo><mn>34</mn><mo>,</mo><msub><mrow><mi>K</mi></mrow><mrow><mi>a</mi></mrow></msub><mo>≤</mo><mn>10</mn></mrow></math></span>) were identified for the first time. The effective model consisted of a <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>6</mn></mrow></msub><mo>+</mo><msub><mrow><mi>ν</mi>
对大气污染物氯二氟甲烷(HCFC-22)的同位素混合物(13C ~ 29.8±0.14%)在779 ~ 849 cm−1范围内的高分辨率红外光谱进行了反振动分析,光谱特征仅限于最丰富的12CH35ClF2和13CH35ClF2。光谱记录在布鲁克IFS-125HR光谱仪上,分辨率为≈0.001 cm−1。采用考虑ν4/ν 2ν6费米共振和ν4/ν6+ν9科里奥利共振的华生a型简化有效哈密顿量(Heff)求解了主同位素体12CH35ClF2的反光谱问题。确定的ν4的3003个跃迁和2ν6的1265个跃迁产生了ν4的1598个经验高能能级(J≤81,Ka≤13)和2ν6的840个经验高能能级(J≤71,Ka≤11),RMSD = 2.92×10−4 cm−1。对于13CH35ClF2同位素,首次发现了670个跃迁和对应的ν4波段(J≤34,Ka≤10)的350个经验能级。有效模型由ν4/ν6+ν9相互作用双元组成,再现的经验能级RMSD=4.97×10−4 cm−1。利用四阶Van Vleck算子摄动理论CVPT(4)与CCSD(T)/cc-pVTZ &; CCSD(T)/ augg -cc- pv (Q+d)Z势能和偶极矩混合曲面得到的自定义有效偶极矩算子计算振动-旋转跃迁的理论强度,大大简化了所研究的高拥塞谱的分配。实验光谱的解密使用Python软件包和广泛的可视化图形工具进行。
{"title":"High-resolution ro-vibrational analysis of HCFC-22: Deciphering ν4 and 2ν6 bands of 12CH35ClF2 and ν4 band of 13CH35ClF2 species","authors":"Egor O. Dobrolyubov ,&nbsp;Ilya M. Efremov ,&nbsp;Sergey V. Krasnoshchekov ,&nbsp;Igor V. Polyakov ,&nbsp;Vladimir B. Laptev ,&nbsp;Sergey A. Klimin ,&nbsp;Dmitry V. Millionshchikov ,&nbsp;Olga V. Naumenko","doi":"10.1016/j.jqsrt.2025.109721","DOIUrl":"10.1016/j.jqsrt.2025.109721","url":null,"abstract":"&lt;div&gt;&lt;div&gt;A ro-vibrational analysis of a high-resolution IR spectrum of an isotopic mixture of the atmospheric pollutant chlorodifluoromethane (HCFC-22), enriched in &lt;sup&gt;13&lt;/sup&gt;C to 29.8 ± 0.14%, was performed in the range of 779–849 cm&lt;sup&gt;−1&lt;/sup&gt;, and the identification of spectral features was limited to most abundant species &lt;sup&gt;12&lt;/sup&gt;CH&lt;sup&gt;35&lt;/sup&gt;ClF2 and &lt;sup&gt;13&lt;/sup&gt;CH&lt;sup&gt;35&lt;/sup&gt;ClF&lt;sub&gt;2&lt;/sub&gt;. The spectrum was recorded on a Bruker IFS-125HR FT spectrometer at room temperature with a resolution of &lt;span&gt;&lt;math&gt;&lt;mo&gt;≈&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;0.001 cm&lt;sup&gt;−1&lt;/sup&gt;. The inverse spectroscopic problem for the main isotopologue &lt;sup&gt;12&lt;/sup&gt;CH&lt;sup&gt;35&lt;/sup&gt;ClF&lt;sub&gt;2&lt;/sub&gt; was solved with Watson-type &lt;span&gt;&lt;math&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;-reduced effective Hamiltonian (&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;eff&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;) with accounting of 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;mn&gt;2&lt;/mn&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; Fermi resonance and 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;6&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;9&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; Coriolis resonance. The identified 3003 transitions of &lt;span&gt;&lt;math&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;/math&gt;&lt;/span&gt; and 1265 transitions of &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; produced 1598 empirical upper energy levels of the &lt;span&gt;&lt;math&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;/math&gt;&lt;/span&gt; (&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;J&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;81&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;K&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;13&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;) and 840 levels of the &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; band (&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;J&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;71&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;K&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;) with RMSD = 2.92&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; cm&lt;sup&gt;−1&lt;/sup&gt;. For the &lt;sup&gt;13&lt;/sup&gt;CH&lt;sup&gt;35&lt;/sup&gt;ClF&lt;sub&gt;2&lt;/sub&gt; isotopologue, 670 transitions and corresponding empirical 350 energy levels of &lt;span&gt;&lt;math&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;/math&gt;&lt;/span&gt; band (&lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;J&lt;/mi&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;34&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;K&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;≤&lt;/mo&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;) were identified for the first time. The effective model consisted of a &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;6&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;","PeriodicalId":16935,"journal":{"name":"Journal of Quantitative Spectroscopy & Radiative Transfer","volume":"348 ","pages":"Article 109721"},"PeriodicalIF":1.9,"publicationDate":"2025-10-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145412040","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
Investigation of ultraviolet spectrum and energy level assignments of Gd I in the 305–325nm region Gd I在305-325 nm区域的紫外光谱和能级分配研究
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-10-31 DOI: 10.1016/j.jqsrt.2025.109731
Yun-Fei Li , Jun-Yao Zhang , Jing-Yi Xiong , Kai-Chen Ma , Li-De Wang , Cai-Hua Zhu
The ultraviolet spectrum of Gd I in the 305–325 nm range was studied using resonance ionization spectroscopy, revealing 196 transition lines, including 66 strong ones. The lower and upper energy levels were assigned to 190 lines by combining available reference data with pump–probe verification, 172 of which are reported for the first time. Seventeen new even-parity high-lying excited states were also identified. The strong lines reported here will contribute to future studies of Gd I Rydberg and autoionization states and enable two-color, two-step photoionization pathways for isotope separation and resonance ionization mass spectrometry analysis.
利用共振电离光谱研究了Gd I在305 ~ 325 nm范围内的紫外光谱,共发现196条过渡谱线,其中强过渡谱线66条。结合现有参考数据和泵-探针验证,对190条管线进行了上下能级划分,其中172条管线为首次报告。还发现了17个新的偶宇称高位激发态。本文报道的强谱线将有助于未来Gd I Rydberg和自电离态的研究,并为同位素分离和共振电离质谱分析提供双色、两步光电离途径。
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引用次数: 0
Corrigendum to “A practical guide to coding line-by-line trace gas absorption in Earth's atmosphere” [Journal of Quantitative Spectroscopy & Radiative Transfer 337 (2025) 109345] “对地球大气中逐行微量气体吸收进行编码的实用指南”的勘误表[定量光谱学与辐射传输杂志337 (2025)109345]
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-10-30 DOI: 10.1016/j.jqsrt.2025.109713
S. Korkin , A.M. Sayer , A. Ibrahim , A. Lyapustin
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引用次数: 0
Tuning the electromagnetic density spectral function in a graphene–dielectric micro-cavity 石墨烯-介电介质微腔中电磁密度谱函数的调谐
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-10-28 DOI: 10.1016/j.jqsrt.2025.109716
Julieta Olivo , Hernán Ferrari , Jorge L. Blengino Albrieu , Mauro Cuevas
This work focuses on the study of the electromagnetic density spectral function (DSF) near a graphene–dielectric cavity. The cavity is formed in the space confined by the base of a dielectric micro-cube and a planar graphene sheet covering a dielectric substrate. The size and refractive index of the micro-cube, the constitutive parameters of graphene, and the gap between the dielectric cube and the graphene sheet determine the modifications to the DSF. We have developed a method based on the coupled dipole approximation (CDA), incorporating the surface Green’s tensor to account for the scattering processes with the graphene substrate, thereby rigorously modeling the electromagnetic problem. Our results reveal three well-distinguishable peaks in the DSF spectrum, which are attributed to the isolated micro-cube, the graphene substrate, and their mutual interaction. Specific parameters allow for the selective tuning of an individual peak’s properties, with minimal crosstalk to other spectral features. Using simple physical arguments related to the kinetic characteristics of surface plasmons (SPs) on graphene, we explain the key dependencies on constitutive and geometrical parameters.
本文主要研究石墨烯介电腔附近的电磁密度谱函数(DSF)。该空腔形成于由介电微立方体的基底和覆盖介电衬底的平面石墨烯片所限制的空间中。微立方体的尺寸和折射率、石墨烯的本构参数以及介质立方体与石墨烯片之间的间隙决定了对DSF的修改。我们开发了一种基于耦合偶极子近似(CDA)的方法,结合表面格林张量来解释石墨烯衬底的散射过程,从而严格模拟电磁问题。我们的研究结果揭示了DSF光谱中三个很好区分的峰,这归因于孤立的微立方体,石墨烯衬底及其相互作用。特定的参数允许对单个峰的属性进行选择性调谐,并且对其他光谱特征的串扰最小。使用与石墨烯表面等离子体(SPs)的动力学特性相关的简单物理参数,我们解释了本构和几何参数的关键依赖关系。
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引用次数: 0
First high-resolution spectral study of the far infrared fundamental OH- torsional band of ethyl alcohol (CH3CH2OH), using synchrotron radiation 首次使用同步辐射对乙醇(CH3CH2OH)的远红外基羟基扭带进行高分辨率光谱研究
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-10-27 DOI: 10.1016/j.jqsrt.2025.109707
Indranath Mukhopadhyay
In this work, the high-resolution far infrared (FIR) and infrared (IR) spectrum of ethyl alcohol has been recorded in the range 50–1200 cm-1, with an excellent signal-to-noise (S/N) ratio, using a synchrotron radiation-based Fourier transform spectrometer. This spectrum, along with the spectrum obtained earlier with a conventional Fourier transform spectrometer in the range 15–350 cm-1, has been utilized to assign many ∆K=±1 transitions from the trans- or anti and gauche-states in the ground state to connect the lowest lying state (o2) for the first excited OH torsional vibrational band. Since the transitions originating from the trans- states are the strongest mode, the terminating state is termed trans (anti) State (o2). However, this state has odd parity. In addition, many millimeter (MMW) wave transitions have been measured elsewhere and assigned. The assignments have been rigorously confirmed using several complementary methods. An expanded appendix (Appendix-1) of about 8000 accurate wavenumbers of assigned transitions in the millimeter (MMW), FIR, and IR regions has been prepared and is being submitted as a depository. The assignments allowed indirect energy differences between the trans- and gauche states in the ground state, which are not otherwise obtainable via dipole selection rules. The accurate wavenumbers should help detect ethanol in interstellar space, particularly using the IR telescopes, and for further studies on intricate interactions between the various vibrational modes and rotation. This is the first time high-resolution studies have been performed in the elusive excited torsional state of ethyl alcohol. The reported transition wavenumber should have an uncertainty of less than ±0.0002 cm-1
在这项工作中,使用基于同步辐射的傅立叶变换光谱仪,在50-1200 cm-1范围内记录了乙醇的高分辨率远红外(FIR)和红外(IR)光谱,具有良好的信噪比(S/N)。该光谱与之前使用传统傅立叶变换光谱仪在15-350 cm-1范围内获得的光谱一起,已被用于分配基态中反或反和扭扭态的许多∆K=±1跃迁,以连接第一个激发OH扭转振动带的最低分布态(o2)。由于源自反态的跃迁是最强的模式,终止态被称为反态(o2)。然而,这种状态有奇偶校验。此外,许多毫米波跃迁已经在其他地方测量和分配。用几种互补的方法对赋值进行了严格的确认。已经编制了一个扩展附录(附录-1),其中包含了毫米(MMW)、FIR和IR区域中约8000个精确的指定跃迁波数,并正在作为存档提交。这种分配允许在基态的反式态和间扭态之间存在间接的能量差异,这是通过偶极子选择规则无法获得的。准确的波数应该有助于探测星际空间中的乙醇,特别是使用红外望远镜,以及进一步研究各种振动模式和旋转之间复杂的相互作用。这是首次在难以捉摸的乙醇激发态中进行高分辨率研究。报告的跃迁波数的不确定度应小于±0.0002 cm-1
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引用次数: 0
Theoretical studies of allowed (E1) and forbidden (E2) transitions in Zr+29 Zr + 29中允许(E1)和禁止(E2)跃迁的理论研究
IF 1.9 3区 物理与天体物理 Q2 OPTICS Pub Date : 2025-10-27 DOI: 10.1016/j.jqsrt.2025.109719
S. Eser , G. Günday Konan , B. Karaçoban Usta , İ. Gülsoy
In this study, level energies, their radiative lifetimes and Landé g-factors, wavelengths, transition probabilities, weighted oscillator strengths and line strengths for electric dipole (E1) and electric quadrupole (E2) transitions of sodium-like zirconium (Zr+29(Zr XXX), Z = 40) are determined. Four atomic codes are used in the calculations: the pseudo-relativistic Hartree–Fock code, including superposition of configurations with relativistic corrections (Cowan’s HFR method), the multiconfiguration Hartree–Fock (MCHF) method within the framework of Breit–Pauli relativistic corrections, the AUTOSTRUCTURE code, which includes Breit interactions and quantum electrodynamics contributions, and the general-purpose relativistic atomic structure package (GRASP) based on a fully relativistic multiconfiguration Dirac–Fock (MCDF) method. Our data set is compared with other results available in the literature. Furthermore, we present new atomic data for Zr+29, which have not been published previously. The present results are reported as reference points for future calculations and measurements.
本研究确定了类钠锆(Zr+29(Zr XXX), Z = 40)电偶极子(E1)和电四极子(E2)跃迁的能级能、辐射寿命和land g因子、波长、跃迁概率、加权振子强度和线强度。计算中使用了四种原子代码:伪相对论Hartree-Fock代码,包括带相对论修正的组态叠加(Cowan的HFR方法),Breit - pauli相对论修正框架内的多组态Hartree-Fock (MCHF)方法,AUTOSTRUCTURE代码,包括Breit相互作用和量子电动力学贡献,以及基于完全相对论多组态Dirac-Fock (MCDF)方法的通用相对论原子结构包(GRASP)。我们的数据集与文献中其他可用的结果进行了比较。此外,我们提出了Zr+29的新原子数据,这是以前没有发表过的。本报告的结果作为今后计算和测量的参考点。
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引用次数: 0
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Journal of Quantitative Spectroscopy & Radiative Transfer
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