Pub Date : 2025-01-15DOI: 10.1140/epjd/s10053-024-00950-3
Chong Lv, Jialun Chai, Xiaona Ban, Wei Sun
This study focuses on optimizing beam driving modes to enhance laser-target coupling efficiency and improve particle quality in laser-driven ion acceleration. The aim is to increase proton and ion beam energy. Two-dimensional particle-in-cell simulations are conducted to investigate the proton beam generated by a Petawatt laser-driven multilayer target. The results indicate that optimal space overlap between the laser and targets improves energy coupling efficiency. Numerical simulation results indicate that the overlap of two laser pulses in front of the target, specifically at the same focal point, results in the generation of higher-energy ion beams. This result is primarily attributed to the enhanced longitudinal electric field under such conditions, which leads to increased energies of protons and ions. By adjusting the longitudinal size of the CH layer, a high-quality proton beam with a maximum cut-off energy of approximately 290 MeV and a small energy spread of 5.2(%) and 14.7(%) is achieved
{"title":"Study on the coupling and ion acceleration between ultraintense laser and multilayer solid targets","authors":"Chong Lv, Jialun Chai, Xiaona Ban, Wei Sun","doi":"10.1140/epjd/s10053-024-00950-3","DOIUrl":"10.1140/epjd/s10053-024-00950-3","url":null,"abstract":"<p>This study focuses on optimizing beam driving modes to enhance laser-target coupling efficiency and improve particle quality in laser-driven ion acceleration. The aim is to increase proton and ion beam energy. Two-dimensional particle-in-cell simulations are conducted to investigate the proton beam generated by a Petawatt laser-driven multilayer target. The results indicate that optimal space overlap between the laser and targets improves energy coupling efficiency. Numerical simulation results indicate that the overlap of two laser pulses in front of the target, specifically at the same focal point, results in the generation of higher-energy ion beams. This result is primarily attributed to the enhanced longitudinal electric field under such conditions, which leads to increased energies of protons and ions. By adjusting the longitudinal size of the CH layer, a high-quality proton beam with a maximum cut-off energy of approximately 290 MeV and a small energy spread of 5.2<span>(%)</span> and 14.7<span>(%)</span> is achieved</p>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"79 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2025-01-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142994547","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 : 2025-01-08DOI: 10.1140/epjd/s10053-024-00945-0
Hongfeng Zheng, Die Fang, Liguang Jiao, Xiaolei Che, Zhenwen Dai
We utilized the archival data recorded by the Fourier transform spectrometer at the USA National Solar Observatory to investigate the hyperfine structure (HFS) for neutral manganese (Mn I) and singly ionized manganese (Mn II) levels. HFS constants for 25 levels of Mn I between 24,779 cm−1 and 62,671 cm−1 and, those for 14 levels of Mn II between 38,366 cm−1 and 99,893 cm−1 were determined by analyzing 100 spectral lines, among which the results for 15 levels of Mn I and eight levels of Mn II are reported for the first time, to our best knowledge. This increases the total number of levels with experimental HFS constants to 182 for Mn I and 116 for Mn II. For two Mn I levels and one Mn II level, both magnetic dipole HFS constants A and electric quadrupole HFS constants B were obtained. For the other levels, only A constants were determined. The uncertainties of most of the HFS constants determined in this work are less than 10%.
{"title":"Hyperfine structure constants for neutral and singly ionized manganese using Fourier transform spectra","authors":"Hongfeng Zheng, Die Fang, Liguang Jiao, Xiaolei Che, Zhenwen Dai","doi":"10.1140/epjd/s10053-024-00945-0","DOIUrl":"10.1140/epjd/s10053-024-00945-0","url":null,"abstract":"<div><p><b>We utilized the archival data recorded by the Fourier transform spectrometer at the USA National Solar Observatory to investigate the hyperfine structure (HFS) for neutral manganese (Mn I) and singly ionized manganese (Mn II) levels.</b> HFS constants for 25 levels of Mn I between 24,779 cm<sup>−1</sup> and 62,671 cm<sup>−1</sup> and, those for 14 levels of Mn II between 38,366 cm<sup>−1</sup> and 99,893 cm<sup>−1</sup> were determined by analyzing 100 spectral lines, among which the results for 15 levels of Mn I and eight levels of Mn II are reported for the first time, to our best knowledge. <b>This increases the total number of levels with experimental HFS constants to 182 for Mn I and 116 for Mn II.</b> For two Mn I levels and one Mn II level, both magnetic dipole HFS constants <i>A</i> and electric quadrupole HFS constants <i>B</i> were obtained. For the other levels, only <i>A</i> constants were determined. The uncertainties of most of the HFS constants determined in this work are less than 10%.</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":"79 1","pages":""},"PeriodicalIF":1.5,"publicationDate":"2025-01-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142939198","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 : 2024-12-23DOI: 10.1140/epjd/s10053-024-00946-z
Fellype do Nascimento, Kleber A. Petroski, Thalita M. C. Nishime, Konstantin G. Kostov
Atmospheric pressure plasma jets (APPJs) are versatile devices with numerous applications. This work focuses on APPJs generated at the tip of long, flexible tubes using the jet transfer technique. The plasma source consists of a primary discharge and a secondary discharge forming the plasma jet. Discharge power measurements were carried out in a way that it was possible to separate the contribution of the primary discharge from the total power dissipated by the plasma source. Both power and effective current were analyzed under different operating conditions. The results show that the variation in the primary discharge power is much lower than the power dissipated by the plasma jet. Additionally, the electrical characteristics of the plasma device were analyzed. Notable differences were observed between the negative and positive phases of the discharge, with a more resistive load in the negative one, which suggests that the electrical equivalent circuit model changes according to the voltage polarity.
The primary discharge spectra are not affected by differences in electrical characteristics of the discharges with the plasma jet on and off
{"title":"Measurements of power dissipated in an atmospheric pressure plasma jet device with double plasma discharge ignition","authors":"Fellype do Nascimento, Kleber A. Petroski, Thalita M. C. Nishime, Konstantin G. Kostov","doi":"10.1140/epjd/s10053-024-00946-z","DOIUrl":"10.1140/epjd/s10053-024-00946-z","url":null,"abstract":"<p>Atmospheric pressure plasma jets (APPJs) are versatile devices with numerous applications. This work focuses on APPJs generated at the tip of long, flexible tubes using the jet transfer technique. The plasma source consists of a primary discharge and a secondary discharge forming the plasma jet. Discharge power measurements were carried out in a way that it was possible to separate the contribution of the primary discharge from the total power dissipated by the plasma source. Both power and effective current were analyzed under different operating conditions. The results show that the variation in the primary discharge power is much lower than the power dissipated by the plasma jet. Additionally, the electrical characteristics of the plasma device were analyzed. Notable differences were observed between the negative and positive phases of the discharge, with a more resistive load in the negative one, which suggests that the electrical equivalent circuit model changes according to the voltage polarity.</p><p>The primary discharge spectra are not affected by differences in electrical characteristics of the discharges with the plasma jet on and off</p>","PeriodicalId":789,"journal":{"name":"The European Physical Journal D","volume":"78 12","pages":""},"PeriodicalIF":1.5,"publicationDate":"2024-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142875213","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 : 2024-12-20DOI: 10.1140/epjd/s10053-024-00944-1
Muhammad Fahad, Khizar Hussain Shah, Sajjad Ali, Muhammad Abrar
Precise determination of heavy metals and trace elements in eggshells from conventional and organic poultry production systems is carried out using a two distinct CF-LIBS techniques, namely one-line calibration-free (OLCF) and self-calibration (SC) LIBS, coupled with XRD, WD-XRF, EDS and FTIR. A Q-switched Nd:YAG laser with a wavelength of 1064 nm, pulse duration of 9 ns and pulse energy of 126 mJ was used to generate plasma. Spectral analysis revealed Ca, Mg, S, Fe, Mn, Cr, Sr, Al, Cu, Ni, Na, and Li in both organic (OE) and regular (FE) chicken eggshells, whereas a heavy element Ba was only detected in OE emission spectra. A mean value of plasma temperature was calculated as 7500 ± 750 K using a Boltzmann plot in addition to Saha-Boltzmann plot approach with self-absorption corrections and used for calcium quantification, whereas electron number density value was calculated as 5.68 × 1016 cm−3. The concentration of major constituent Ca in OE versus FE determined by CF-LIBS techniques along with XRF and EDS was found as: OLCF-LIBS = 99.23% versus 99.11%, SC-LIBS = 99.78% versus 99.73%, XRF = 99.81% versus 99.76%, and EDS = 99.83% versus 99.89%. The results showed that SC-LIBS method is more accurate for precise compositional analysis and findings were close to that determined by XRF and EDS methods. The results further demonstrated LIBS capability to identify heavy metals and trace elements within eggshell samples accurately and hence, contributing to and advancing our understanding of the utilization of LIBS technique in this field.