Pub Date : 2025-11-15DOI: 10.1007/s00340-025-08596-8
A. K. Poteomkin, M. A. Martyanov, I. V. Kuzmin, E. I. Gacheva, S.Yu. Mironov, E. A. Khazanov
Values of all four elements of the cubic susceptibility in KDP and DKDP (80% deuteration) crystals at wavelengths of 1030 and 515 nm were measured for the first time by the modified z-scan technique. Values of the tensor elements (chi _{11}), (chi _{16}), and (chi _{33}) are approximately the same for the considered crystals. The value of the effective cubic susceptibility in the DKDP ((Z-)cut) crystal does not depend on the azimuthal angle of rotation in contrast of KDP crystal at the experimental measurement accuracy. Thus the values of tensor elements (chi _{18}) are different in both crystals.
在KDP和DKDP中立方磁化率的所有四个元素的值(80% deuteration) crystals at wavelengths of 1030 and 515 nm were measured for the first time by the modified z-scan technique. Values of the tensor elements (chi _{11}), (chi _{16}), and (chi _{33}) are approximately the same for the considered crystals. The value of the effective cubic susceptibility in the DKDP ((Z-)cut) crystal does not depend on the azimuthal angle of rotation in contrast of KDP crystal at the experimental measurement accuracy. Thus the values of tensor elements (chi _{18}) are different in both crystals.
{"title":"Determining all elements of cubic nonlinearity susceptibility tensor in KDP and DKDP crystals","authors":"A. K. Poteomkin, M. A. Martyanov, I. V. Kuzmin, E. I. Gacheva, S.Yu. Mironov, E. A. Khazanov","doi":"10.1007/s00340-025-08596-8","DOIUrl":"10.1007/s00340-025-08596-8","url":null,"abstract":"<div><p>Values of all four elements of the cubic susceptibility in KDP and DKDP (80% deuteration) crystals at wavelengths of 1030 and 515 nm were measured for the first time by the modified z-scan technique. Values of the tensor elements <span>(chi _{11})</span>, <span>(chi _{16})</span>, and <span>(chi _{33})</span> are approximately the same for the considered crystals. The value of the effective cubic susceptibility in the DKDP (<span>(Z-)</span>cut) crystal does not depend on the azimuthal angle of rotation in contrast of KDP crystal at the experimental measurement accuracy. Thus the values of tensor elements <span>(chi _{18})</span> are different in both crystals.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":"131 12","pages":""},"PeriodicalIF":2.0,"publicationDate":"2025-11-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145561060","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}
Pub Date : 2025-11-15DOI: 10.1007/s00340-025-08560-6
Martin Richter, Johannes Lill, Robert S. Barlow, James R. Dawson, Andreas Dreizler, Dirk Geyer
Quantitative measurements of minor species are essential for understanding flame propagation and emission formation, and for validation of chemical kinetic models. Laser-induced fluorescence-based methods are widely employed due to their ability to selectively excite specific species and achieve high signal-to-noise ratios. However, these techniques are inherently susceptible to collisional quenching, which complicates signal quantification. Bi-directional laser-induced fluorescence (BD-LIF) was proposed decades ago as a promising approach to obtain absolute species concentrations while preserving spatial resolution. Despite its potential, initial measurements showed deviations of 50 – 60 % compared to equilibrium calculations and 1D simulations. We present a generalized quantification strategy for BD-LIF based on the general form of Beer’s law that explicitly accounts for wavenumber-dependent absorption and the resulting spatial evolution of the overlap between laser and absorption line, due to the stronger absorption near the line center. The method is demonstrated by measuring hydroxyl (OH) radicals following excitation in the A–X(1,0) system in the post-flame region of laminar CH4-air flames. The results show very good agreement with simulated OH concentrations, underscoring the robustness of the generalized approach and its potential for broader application in combustion diagnostics.
{"title":"A generalized quantification method for bi-directional laser-induced fluorescence","authors":"Martin Richter, Johannes Lill, Robert S. Barlow, James R. Dawson, Andreas Dreizler, Dirk Geyer","doi":"10.1007/s00340-025-08560-6","DOIUrl":"10.1007/s00340-025-08560-6","url":null,"abstract":"<div><p>Quantitative measurements of minor species are essential for understanding flame propagation and emission formation, and for validation of chemical kinetic models. Laser-induced fluorescence-based methods are widely employed due to their ability to selectively excite specific species and achieve high signal-to-noise ratios. However, these techniques are inherently susceptible to collisional quenching, which complicates signal quantification. Bi-directional laser-induced fluorescence (BD-LIF) was proposed decades ago as a promising approach to obtain absolute species concentrations while preserving spatial resolution. Despite its potential, initial measurements showed deviations of 50 – 60 % compared to equilibrium calculations and 1D simulations. We present a generalized quantification strategy for BD-LIF based on the general form of Beer’s law that explicitly accounts for wavenumber-dependent absorption and the resulting spatial evolution of the overlap between laser and absorption line, due to the stronger absorption near the line center. The method is demonstrated by measuring hydroxyl (OH) radicals following excitation in the A–X(1,0) system in the post-flame region of laminar CH<sub>4</sub>-air flames. The results show very good agreement with simulated OH concentrations, underscoring the robustness of the generalized approach and its potential for broader application in combustion diagnostics.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":"131 12","pages":""},"PeriodicalIF":2.0,"publicationDate":"2025-11-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s00340-025-08560-6.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145511146","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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}
Pub Date : 2025-11-15DOI: 10.1007/s00340-025-08588-8
Deyue An, Yuanhao Du, Xing Kong, Lian Zhu, Hui Feng, Shuai Wu
This study proposes a novel technique for rapid three-dimensional (3D) reconstruction based on pulsed terahertz inverse synthetic aperture radar (ISAR), addressing the critical bottleneck of low reconstruction efficiency in terahertz time-domain spectroscopy (THz-TDS) ISAR systems for non-destructive testing (NDT) applications. By introducing the Range Migration Algorithm (RMA) and Phase Shift Migration Algorithm (PSMA) into 3D imaging processing, with specialized calibration and adaptation for the ultra-wide bandwidth and poor amplitude flatness characteristics of pulsed terahertz signals, we systematically compare their performance with the conventional time-domain Back-Projection Algorithm (BPA) in terms of imaging quality and computational efficiency. Experimental results demonstrate that RMA and PSMA maintain high imaging quality (SNR ≥ 25 dB, MAE < 6.5 dB, SSIM between 0.72 and 0.90, lateral resolution of 0.3 mm, and range resolution of 0.08 mm) while reducing single-image reconstruction time from several hours to minutes-achieving computational efficiency of only 1–2% compared to Graphics Processing Unit (GPU) accelerated BPA. Through non-destructive imaging of practical objects such as thermocouple plugs and integrated circuit (IC) keychain cards, the system clearly reveals submillimeter surface structures, internal screws, and copper coil arrangements, validating its exceptional performance and engineering application potential in 3D imaging for NDT.
{"title":"Terahertz ISAR non-destructive testing technology based on THz-TDS with fast reconstruction","authors":"Deyue An, Yuanhao Du, Xing Kong, Lian Zhu, Hui Feng, Shuai Wu","doi":"10.1007/s00340-025-08588-8","DOIUrl":"10.1007/s00340-025-08588-8","url":null,"abstract":"<div><p>This study proposes a novel technique for rapid three-dimensional (3D) reconstruction based on pulsed terahertz inverse synthetic aperture radar (ISAR), addressing the critical bottleneck of low reconstruction efficiency in terahertz time-domain spectroscopy (THz-TDS) ISAR systems for non-destructive testing (NDT) applications. By introducing the Range Migration Algorithm (RMA) and Phase Shift Migration Algorithm (PSMA) into 3D imaging processing, with specialized calibration and adaptation for the ultra-wide bandwidth and poor amplitude flatness characteristics of pulsed terahertz signals, we systematically compare their performance with the conventional time-domain Back-Projection Algorithm (BPA) in terms of imaging quality and computational efficiency. Experimental results demonstrate that RMA and PSMA maintain high imaging quality (SNR ≥ 25 dB, MAE < 6.5 dB, SSIM between 0.72 and 0.90, lateral resolution of 0.3 mm, and range resolution of 0.08 mm) while reducing single-image reconstruction time from several hours to minutes-achieving computational efficiency of only 1–2% compared to Graphics Processing Unit (GPU) accelerated BPA. Through non-destructive imaging of practical objects such as thermocouple plugs and integrated circuit (IC) keychain cards, the system clearly reveals submillimeter surface structures, internal screws, and copper coil arrangements, validating its exceptional performance and engineering application potential in 3D imaging for NDT.</p></div>","PeriodicalId":474,"journal":{"name":"Applied Physics B","volume":"131 12","pages":""},"PeriodicalIF":2.0,"publicationDate":"2025-11-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145511090","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}