This study explores the potential for high-harmonic generation (HHG) from argon atomic gas and single attosecond pulse generation by leveraging amplified and hyper-focused short laser pulses through a plasmonic nanostructure. The plasmonic nanostructure features triangular nanobowties with multilayer compositions of dielectrics and metals, supported by an insulating substrate. Within the nanobowtie gap, localized surface plasmons significantly enhance the laser field intensity over a substantial volume of the gap. Fine-tuning the geometric parameters of this structure achieves up to 45-fold amplification (< 17 dB) within the central wavelength of 800 nm of a standard titanium–sapphire laser. This enhancement enables the argon atoms introduced via a gas jet to exhibit a pronounced nonlinear response, leading to high-intensity HHG under incident pulses of relatively low intensity (1012 W/cm2). Based on the harmonic spectrum observed, the generation of isolated attosecond pulses with a temporal width of 33.37 attoseconds is achievable, notably without necessitating chirp mitigation techniques.
{"title":"Attosecond pulse generation using high-order harmonic generation in argon gas based on the enhancement effect of multilayer plasmonics","authors":"Sakineh Nazarpoor, Masoud Mohebbi, Abdolrahim Baharvand","doi":"10.1140/epjd/s10053-025-01109-4","DOIUrl":"10.1140/epjd/s10053-025-01109-4","url":null,"abstract":"<div><p>This study explores the potential for high-harmonic generation (HHG) from argon atomic gas and single attosecond pulse generation by leveraging amplified and hyper-focused short laser pulses through a plasmonic nanostructure. The plasmonic nanostructure features triangular nanobowties with multilayer compositions of dielectrics and metals, supported by an insulating substrate. Within the nanobowtie gap, localized surface plasmons significantly enhance the laser field intensity over a substantial volume of the gap. Fine-tuning the geometric parameters of this structure achieves up to 45-fold amplification (< 17 dB) within the central wavelength of 800 nm of a standard titanium–sapphire laser. This enhancement enables the argon atoms introduced via a gas jet to exhibit a pronounced nonlinear response, leading to high-intensity HHG under incident pulses of relatively low intensity (10<sup>12</sup> W/cm<sup>2</sup>). Based on the harmonic spectrum observed, the generation of isolated attosecond pulses with a temporal width of 33.37 attoseconds is achievable, notably without necessitating chirp mitigation techniques.</p><h3>Graphical abstract</h3><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div></div>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"80 2","pages":""},"PeriodicalIF":1.5,"publicationDate":"2026-01-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146083206","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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}
The behavior of toroidal and poloidal rotations in the edge region is studied in the presence of locked m/n = 2/1 and m/n = 3/1 magnetic islands, excited by Resonant Magnetic Perturbations (RMPs) on the J-TEXT tokamak. When the 2/1 magnetic island is present, a significant change in the toroidal rotation of carbon V (C4+) is observed, with the reversing from the counter-current to the co-current direction. In contrast, the 3/1 magnetic island has a weaker effect on C4+ rotation but strongly influences the rotation of carbon III (C2+), which is closer to the 3/1 island. RMP phase scans show that the toroidal rotation change of C2+ increases as it approaches the O-point of the magnetic island. This region corresponds to a more positive radial electric field Er on the outer side of the 3/1 magnetic island, as measured by electric probes.
Graphical abstract
Evolution of CV toroidal rotation measured by different viewing channels when 2/1 magnetic islands are induced at different phases
Evolutions of C III toroidal rotation under different RMP phases measured from 2 different directions when 3/1 magnetic islands are induced at different phases. Red solid line represent measurement from counter-Ip direction and blue represent co-Ip direction
{"title":"Impact of magnetic islands on edge plasma rotation in J-TEXT tokamak","authors":"Xiaoyi Zhang, Zhifeng Cheng, Wei Yan, Zhipeng Chen, Zhoujun Yang, Song Zhou, Zezhi Yu, Zhengkang Ren, Yonghua Ding","doi":"10.1140/epjd/s10053-026-01118-x","DOIUrl":"10.1140/epjd/s10053-026-01118-x","url":null,"abstract":"<div><p>The behavior of toroidal and poloidal rotations in the edge region is studied in the presence of locked m/n = 2/1 and m/n = 3/1 magnetic islands, excited by Resonant Magnetic Perturbations (RMPs) on the J-TEXT tokamak. When the 2/1 magnetic island is present, a significant change in the toroidal rotation of carbon V (C<sup>4+</sup>) is observed, with the reversing from the counter-current to the co-current direction. In contrast, the 3/1 magnetic island has a weaker effect on C<sup>4+</sup> rotation but strongly influences the rotation of carbon III (C<sup>2+</sup>), which is closer to the 3/1 island. RMP phase scans show that the toroidal rotation change of C<sup>2+</sup> increases as it approaches the O-point of the magnetic island. This region corresponds to a more positive radial electric field E<sub>r</sub> on the outer side of the 3/1 magnetic island, as measured by electric probes.</p><h3>Graphical abstract</h3><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div><p>Evolution of CV toroidal rotation measured by different viewing channels when 2/1 magnetic islands are induced at different phases</p><div><figure><div><div><picture><source><img></source></picture></div></div></figure></div><p>Evolutions of C III toroidal rotation under different RMP phases measured from 2 different directions when 3/1 magnetic islands are induced at different phases. Red solid line represent measurement from counter-<i>I</i><sub><i>p</i></sub> direction and blue represent co-<i>I</i><sub><i>p</i></sub> direction</p></div>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"80 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2026-01-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146082514","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2026-01-27DOI: 10.1140/epjd/s10053-025-01108-5
Samir A. El-Tantawy, Fazal Wahed, Ata-ur-Rahman, J. Derbali, Hanan Al-Ghamdi, Aljawhara H. Almuqrin
In this study, we examine three-dimensional (3D) modulated ion-acoustic waves (IAWs) and associated multi-rogue waves in a magnetoplasma consisting of kappa-distributed electrons and hot, anisotropic positive ions. By employing a reductive perturbation technique (the derivative expansion method), the fundamental fluid equations are reduced to the three-dimensional nonlinear Schrödinger equation (3D-NLSE) to investigate the 3D modulational instability (3D-MI) and associated modulated IAWs. For the plasma parameters of interest, such as the anisotropic parallel ion pressure, magnetic field (ion gyrofrequency), and the spectral index of the kappa distribution, the stable and unstable regions of modulated envelope structures are precisely identified. The criteria for the 3D-MI based on the 3D-NLSE are determined and numerically examined. Furthermore, the analytical and numerical solutions for first-order and second-order ion-acoustic rogue waves (IARWs) are investigated. The effects of relevant plasma parameters on the IARW profile are also examined. The implications of our findings for specific environments, such as Earth’s magnetosheath and magnetosphere, are also discussed.
Multidimentional MI and RWs in superthermal anisotropic plasma
{"title":"Multidimensional modulational instability and associated multi-rogue waves in anisotropic magnetized superthermal plasmas","authors":"Samir A. El-Tantawy, Fazal Wahed, Ata-ur-Rahman, J. Derbali, Hanan Al-Ghamdi, Aljawhara H. Almuqrin","doi":"10.1140/epjd/s10053-025-01108-5","DOIUrl":"10.1140/epjd/s10053-025-01108-5","url":null,"abstract":"<p>In this study, we examine three-dimensional (3D) modulated ion-acoustic waves (IAWs) and associated multi-rogue waves in a magnetoplasma consisting of kappa-distributed electrons and hot, anisotropic positive ions. By employing a reductive perturbation technique (the derivative expansion method), the fundamental fluid equations are reduced to the three-dimensional nonlinear Schrödinger equation (3D-NLSE) to investigate the 3D modulational instability (3D-MI) and associated modulated IAWs. For the plasma parameters of interest, such as the anisotropic parallel ion pressure, magnetic field (ion gyrofrequency), and the spectral index of the kappa distribution, the stable and unstable regions of modulated envelope structures are precisely identified. The criteria for the 3D-MI based on the 3D-NLSE are determined and numerically examined. Furthermore, the analytical and numerical solutions for first-order and second-order ion-acoustic rogue waves (IARWs) are investigated. The effects of relevant plasma parameters on the IARW profile are also examined. The implications of our findings for specific environments, such as Earth’s magnetosheath and magnetosphere, are also discussed.</p><p>Multidimentional MI and RWs in superthermal anisotropic plasma</p>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"80 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2026-01-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146082405","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2026-01-21DOI: 10.1140/epjd/s10053-025-01113-8
Yufei Sun, Yonggang Yang, Yang Liu, Tiantian Guan, Chenhao Zheng, Jian Song, Yufang Liu
The fluorescence turn-on mechanism of the quinazolinone-based probe HTPQC for selective cysteine (Cys) detection has been theoretically investigated. Electron–hole analysis indicates that HTPQC has a charge transfer distance (D-index) of 4.86 Å, suggesting significant intramolecular charge transfer (ICT). Additionally, the energy levels of the frontier molecular orbitals (FMOs) for both the donor and acceptor components do not support the occurrence of a photoinduced electron transfer (PET) process. These results illustrate that the weak fluorescence of the probe is mainly attributed to ICT, rather than the PET mechanism proposed in previous studies. Upon reaction with Cys, the product HTPQ shows a reduced D-index (4.59 Å) in its enol form, resulting in enhanced fluorescence at 534 nm. Subsequently, the enol form transforms into the keto form via excited-state intramolecular proton transfer (ESIPT), with a low energy barrier of 1.951 kcal mol−1. In the keto form, complete charge separation occurs (D-index = 7.17 Å), and FMO analysis shows that the highest occupied molecular orbital (HOMO) of the acceptor is higher in energy than that of the donor, indicating PET-induced fluorescence quenching of HTPQ. This study provides a novel theoretical explanation for the photophysical mechanism of cysteine detection via the HTPQC probe, offering insights that diverge from previously established explanations.
{"title":"Theoretical investigation of fluorescence turn-on mechanism for cysteine detection by quinazolinone-based probe HTPQC","authors":"Yufei Sun, Yonggang Yang, Yang Liu, Tiantian Guan, Chenhao Zheng, Jian Song, Yufang Liu","doi":"10.1140/epjd/s10053-025-01113-8","DOIUrl":"10.1140/epjd/s10053-025-01113-8","url":null,"abstract":"<p>The fluorescence turn-on mechanism of the quinazolinone-based probe HTPQC for selective cysteine (Cys) detection has been theoretically investigated. Electron–hole analysis indicates that HTPQC has a charge transfer distance (D-index) of 4.86 Å, suggesting significant intramolecular charge transfer (ICT). Additionally, the energy levels of the frontier molecular orbitals (FMOs) for both the donor and acceptor components do not support the occurrence of a photoinduced electron transfer (PET) process. These results illustrate that the weak fluorescence of the probe is mainly attributed to ICT, rather than the PET mechanism proposed in previous studies. Upon reaction with Cys, the product HTPQ shows a reduced D-index (4.59 Å) in its enol form, resulting in enhanced fluorescence at 534 nm. Subsequently, the enol form transforms into the keto form via excited-state intramolecular proton transfer (ESIPT), with a low energy barrier of 1.951 kcal mol<sup>−1</sup>. In the keto form, complete charge separation occurs (D-index = 7.17 Å), and FMO analysis shows that the highest occupied molecular orbital (HOMO) of the acceptor is higher in energy than that of the donor, indicating PET-induced fluorescence quenching of HTPQ. This study provides a novel theoretical explanation for the photophysical mechanism of cysteine detection via the HTPQC probe, offering insights that diverge from previously established explanations.</p>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"80 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2026-01-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146027128","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2026-01-20DOI: 10.1140/epjd/s10053-025-01116-5
LiangNeng Wu
Based on a two-dimensional compressible magnetohydrodynamic (MHD) model, we systematically investigated the individual effects and combined influence of localized out-of-plane antisymmetric flows and the Hall effect on magnetic reconnection dynamics. The results reveal that both the localized out-of-plane antisymmetric flow and the Hall effect rapidly trigger magnetic reconnection, but the maximum achievable energy conversion rate is reduced, indicating that the nonlinear evolution of reconnection in later stages is suppressed. Additionally, the out-of-plane antisymmetric flow suppresses the magnetic island coalescence observed in purely resistive tearing modes. The introduction of the Hall effect can accelerate the merger of magnetic islands within the current sheet. When combined with the out-of-plane antisymmetric flow's influence, it is shown that the interplay between the Hall effect and the z-axis-aligned out-of-plane antisymmetric flow forms magnetic islands within elongated current sheets, thereby inducing additional plasma instabilities. These findings contribute significantly to the understanding of tearing mode instability development under the coupled influences of outflow dynamics and Hall physics in MHD systems.
{"title":"The impact of localized out-of-plane antisymmetric flows and Hall effect on the magnetic reconnection in a compressible plasma","authors":"LiangNeng Wu","doi":"10.1140/epjd/s10053-025-01116-5","DOIUrl":"10.1140/epjd/s10053-025-01116-5","url":null,"abstract":"<p>Based on a two-dimensional compressible magnetohydrodynamic (MHD) model, we systematically investigated the individual effects and combined influence of localized out-of-plane antisymmetric flows and the Hall effect on magnetic reconnection dynamics. The results reveal that both the localized out-of-plane antisymmetric flow and the Hall effect rapidly trigger magnetic reconnection, but the maximum achievable energy conversion rate is reduced, indicating that the nonlinear evolution of reconnection in later stages is suppressed. Additionally, the out-of-plane antisymmetric flow suppresses the magnetic island coalescence observed in purely resistive tearing modes. The introduction of the Hall effect can accelerate the merger of magnetic islands within the current sheet. When combined with the out-of-plane antisymmetric flow's influence, it is shown that the interplay between the Hall effect and the z-axis-aligned out-of-plane antisymmetric flow forms magnetic islands within elongated current sheets, thereby inducing additional plasma instabilities. These findings contribute significantly to the understanding of tearing mode instability development under the coupled influences of outflow dynamics and Hall physics in MHD systems.</p>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"80 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2026-01-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146027039","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"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 : 2026-01-12DOI: 10.1140/epjd/s10053-025-01112-9
Stefano Scotto, Donatella Ciampini, Rémy Battesti, Carlo Rizzo, Ennio Arimondo
High-resolution optical spectroscopy of Rb atoms in an intermediate-Zeeman magnetic field regime is performed. Magnetic fields between 0.05 T and 0.13 T are measured. We introduce a measurement approach based on three-level (Lambda ) systems where the open-loop frequency energy separation is determined by the applied magnetic field. Using this method an accuracy better than 100 ppm is reached in a measurement series. In parallel, on the basis of complementary measurements based on three-level V systems we obtain the first experimental value of the Landé g-factor of the first excited state for (^{85})Rb, (^{85}g_J(5P_{1/2}))=0.66709(7), and for (^{87})Rb, (^{87}g_J(5P_{1/2}))=0.6663(2). Our approach is unprecedented in the literature for Rb.
Experimental results for the Land´e g-factor of the first excited state of Rb
{"title":"Rb vapour Zeeman optical spectroscopy in a self-calibrated magnetic field","authors":"Stefano Scotto, Donatella Ciampini, Rémy Battesti, Carlo Rizzo, Ennio Arimondo","doi":"10.1140/epjd/s10053-025-01112-9","DOIUrl":"10.1140/epjd/s10053-025-01112-9","url":null,"abstract":"<p>High-resolution optical spectroscopy of Rb atoms in an intermediate-Zeeman magnetic field regime is performed. Magnetic fields between 0.05 T and 0.13 T are measured. We introduce a measurement approach based on three-level <span>(Lambda )</span> systems where the open-loop frequency energy separation is determined by the applied magnetic field. Using this method an accuracy better than 100 ppm is reached in a measurement series. In parallel, on the basis of complementary measurements based on three-level V systems we obtain the first experimental value of the Landé g-factor of the first excited state for <span>(^{85})</span>Rb, <span>(^{85}g_J(5P_{1/2}))</span>=0.66709(7), and for <span>(^{87})</span>Rb, <span>(^{87}g_J(5P_{1/2}))</span>=0.6663(2). Our approach is unprecedented in the literature for Rb.</p><p>Experimental results for the Land´e g-factor of the first excited state of Rb</p>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"80 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2026-01-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjd/s10053-025-01112-9.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145948163","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}
Pub Date : 2025-12-24DOI: 10.1140/epjd/s10053-025-01097-5
Sekhar Dey, Chandan Das, Dipankar Bhattacharyya, Biswajit Ray
This paper presents a study of the phase sensitivity of the transparency and absorption when a microwave (MW) field connects the two ground energy levels of a four-level N-type configuration. This four-level N-type system can be considered with the hyperfine energy levels of the D1 and/or D2 lines of 87Rb atoms. The effect of the MW field on electromagnetically induced transparency (EIT) and on absorption (EIA) is investigated in a weak pump region. Furthermore, we demonstrate that a small absorption dip appears on the top of the EIT in the strong probe region and the absorption dip gradually increases with the increasing value of the MW field at a specific off-detuning position of the pump laser field. The optical Bloch equations for the four-level N-type system are derived and the equations are solved numerically to obtain the results under steady state condition. Additionally, we show that by adjusting the phase of the MW field, a narrow EIT or EIA feature is converted into Autler–Townes Splitting (ATS) under the strong pump conditions.