PHYSICS OF PLASMAS等离子体物理学

PHYSICS OF PLASMAS(英文缩写 PHYS PLASMAS),ISSN 1070-664X,eISSN 1089-7674,中文译名:等离子体物理学 是一本学术期刊。本页汇总该期刊的最新影响因子、分区信息以及最新收录于 PubMed 的文献,帮助您快速了解期刊全貌。

2026 年数据 · 影响因子
2.500
JCR 分区
Q2
CAS 分区
B3
近一年发文量
0
本站 PubMed 收录统计

发文量统计区间:2025-10-01 至 2026-09-30,按本站收录文献的发表日期统计。

ISSN: 1070-664X · eISSN: 1089-7674 · 缩写: PHYS PLASMAS ·中文: 等离子体物理学

期刊介绍

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期刊简介

《Physics of Plasmas》是等离子体物理学领域的核心期刊之一,发表基础等离子体理论、实验与计算研究,覆盖空间与天体物理等离子体、磁约束与惯性约束聚变、低温等离子体、激光等离子体相互作用及等离子体应用等方向。读者主要为等离子体物理、聚变科学、空间物理及相关工程领域的研究人员与研究生,适合展示具有明确物理机制或实验观测价值的系统性工作。

研究方向

主要方向包括磁流体与动理学理论、等离子体不稳定性与湍流、波与粒子相互作用、激光与等离子体相互作用、聚变装置实验、空间与天体等离子体、低温与工业等离子体等。论文类型以原创研究论文为主,兼有综述、快报和评论,强调物理问题的清晰提出与结果的可靠验证。

期刊特色

研究取向偏重物理机制与实验或数值证据的结合,鼓励对已有理论或实验现象提出新解释。论文通常要求方法可复现、结论有明确物理意义,适合从事等离子体物理基础研究、聚变诊断与模拟、空间环境建模等方向的科研人员与高年级研究生阅读和投稿。

投稿难度

投稿难度中等偏上,审稿人重视物理创新性与论证严谨性,而非仅看指标分区。建议在投稿前明确核心物理问题,补充充分的误差分析与对比实验或模拟,并针对等离子体物理社区关注的热点组织讨论;若工作偏工程应用,需突出其基础物理价值。

历年影响因子趋势

JCR 数据年份影响因子JCR 分区
20212.357Q3
20222.200Q3
20232.000Q3
20242.200Q3
20252.500Q2

PHYSICS OF PLASMAS 最新收录文献

  1. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    1. Analytical model of electro-hydrodynamic flow in corona discharge.

    作者:
    Yifei Guan, Ravi Sankar Vaddi, Alberto Aliseda, Igor Novosselov
    日期:
    2018-08-13

    We present an analytical model for electro-hydrodynamic flow that describes the relationship between the corona voltage, electric field, and ion charge density. The interaction between the accelerated ions and the neutral gas molecules is modeled as an external body force in the Navier-Stokes equation. The gas flow characteristics are solved from conservation principles with spectral methods. This multiphysics model is shown to match experimental data for a point-to-ring corona configuration, shedding new insights into mass, charge, and momentum transport phenomena, and can be readily implemented in any numerical simulation.

  2. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    2. Strongly localized magnetic reconnection by the super-Alfvénic shear flow.

    作者:
    Yi-Hsin Liu, M Hesse, F Guo, H Li, T K M Nakamura
    日期:
    2018-08-02

    We demonstrate that the dragging of the magnetic field by the super-Alfvénic shear flows out of the reconnection plane can strongly localize the reconnection x-line in collisionless pair plasmas, reversing the current direction at the x-line. Reconnection with this new morphology, which is impossible in resistive-magnetohydrodynamics, is enabled by the particle inertia. Surprisingly, the quasi-steady reconnection rate remains of order 0.1 even though the aspect ratio of the local x-line geometry is larger than unity, which completely excludes the role of tearing physics. We explain this by examining the transport of the reconnected magnetic flux and the opening angle ma de by the upstream magnetic field, concluding that the reconnection rate is still limited by the constraint imposed at the inflow region. Based on these findings, we propose that this often observed fast rate value of order 0.1 itself, in general, is an upper bound value determined by the upstream constraint, independent of the localization mechanism and dissipation therein.

  3. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    3. Quantifying the Effect of Non-Larmor Motion of Electrons on the Pressure Tensor.

    作者:
    H Che, C Schiff, G Le, J Dorelli, B Giles, T Moore
    日期:
    2018-03-01

    In space plasma, various effects of magnetic reconnection and turbulence cause the electron motion to significantly deviate from their Larmor orbits. Collectively these orbits affect the electron velocity distribution function and lead to the appearance of the "non-gyrotropic" elements in the pressure tensor. Quantification of this effect has important applications in space and laboratory plasma, one of which is tracing the electron diffusion region (EDR) of magnetic reconnection in space observations. Three different measures of agyrotropy of pressure tensor have previously been proposed, namely, ∅ , and . The multitude of contradictory measures has caused confusion within the community. We revisit the problem by considering the basic properties an agyrotropy measure should have. We show that ∅ , and are all defined based on the sum of the principle minors (i.e. the rotation invariant ) of the pressure tensor. We discuss in detail the problems of -based measures and explain why they may produce ambiguous and biased results. We introduce a new measure constructed based on the determinant of the pressure tensor (i.e. the rotation invariant ) which does not suffer from the problems of -based measures. We compare with other measures in 2 and 3-dimension particle-in-cell magnetic reconnection simulations, and show that can effectively trace the EDR of reconnection in both Harris and force-free current sheets. On the other hand, ∅ does not show prominent peaks in the EDR and part of the separatrix in the force-free reconnection simulations, demonstrating that ∅ does not measure all the non-gyrotropic effects in this case, and is not suitable for studying magnetic reconnection in more general situations other than Harris sheet reconnection.

  4. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    4. {"_":"Energy partitioning constraints at kinetic scales in low- turbulence.","i":["β"]}

    作者:
    Daniel J Gershman, Adolfo F-Viñas, John C Dorelli, Melvyn L Goldstein, Jason Shuster, Levon A Avanov, Scott A Boardsen, Julia E Stawarz, Steven J Schwartz, Conrad Schiff, Benoit Lavraud, Yoshifumi Saito, William R Paterson, Barbara L Giles, Craig J Pollock, Robert J Strangeway, Christopher T Russell, Roy B Torbert, Thomas E Moore, James L Burch
    日期:
    2018-02-20

    Turbulence is a fundamental physical process through which energy injected into a system at large scales cascades to smaller scales. In collisionless plasmas, turbulence provides a critical mechanism for dissipating electromagnetic energy. Here we present observations of plasma fluctuations in low- turbulence using data from NASA's Magnetospheric Multiscale mission in Earth's magnetosheath. We provide constraints on the partitioning of turbulent energy density in the fluid, ion-kinetic, and electron-kinetic ranges. Magnetic field fluctuations dominated the energy density spectrum throughout the fluid and ion-kinetic ranges, consistent with previous observations of turbulence in similar plasma regimes. However, at scales shorter than the electron inertial length, fluctuation power in electron kinetic energy significantly exceeded that of the magnetic field, resulting in an electron-motion-regulated cascade at small scales. This dominance should be highly relevant for the study of turbulence in highly magnetized laboratory and astrophysical plasmas.

  5. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    5. Capsule implosions for continuum x-ray backlighting of opacity samples at the National Ignition Facility.

    作者:
    Y P Opachich, R F Heeter, M A Barrios, E M Garcia, R S Craxton, J A King, D A Liedahl, P W McKenty, M B Schneider, M J May, R Zhang, P W Ross, J L Kline, A S Moore, J L Weaver, K A Flippo, T S Perry
    日期:
    2017-06-08

    Direct drive implosions of plastic capsules have been performed at the National Ignition Facility to provide a broad-spectrum (500-2000 eV) X-ray continuum source for X-ray transmission spectroscopy. The source was developed for the high-temperature plasma opacity experimental platform. Initial experiments using 2.0 mm diameter polyalpha-methyl styrene capsules with ∼20 m thickness have been performed. X-ray yields of up to ∼1 kJ/sr have been measured using the Dante multichannel diode array. The backlighter source size was measured to be ∼100 m FWHM, with ∼350 ps pulse duration during the peak emission stage. Results are used to simulate transmission spectra for a hypothetical iron opacity sample at 150 eV, enabling the derivation of photometrics requirements for future opacity experiments.

  6. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    6. First-principles equation-of-state table of beryllium based on density-functional theory calculations.

    作者:
    Y H Ding, S X Hu
    日期:
    2017-06-06

    Beryllium has been considered a superior ablator material for inertial confinement fusion (ICF) target designs. An accurate equation-of-state (EOS) of beryllium under extreme conditions is essential for reliable ICF designs. Based on density-functional theory (DFT) calculations, we have established a wide-range beryllium EOS table of density = 0.001 to 500 g/cm and temperature = 2000 to 10 K. Our first-principle equation-of-state (FPEOS) table is in better agreement with the widely used EOS table ( 2023) than the average-atom and models. For the principal Hugoniot, our FPEOS prediction shows ∼10% stiffer than the last two models in the maximum compression. Although the existing experimental data (only up to 17 Mbar) cannot distinguish these EOS models, we anticipate that high-pressure experiments at the maximum compression region should differentiate our FPEOS from and models. Comparisons between FPEOS and EOS for off-Hugoniot conditions show that the differences in the pressure and internal energy are within ∼20%. By implementing the FPEOS table into the 1-D radiation-hydrodynamic code , we studied the EOS effects on beryllium-shell-target implosions. The FPEOS simulation predicts higher neutron yield (∼15%) compared to the simulation using the 2023 EOS table.

  7. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    7. Numerical analysis of ion temperature effects to the plasma wall transition using a one-dimensional two-fluid model. I. Finite Debye to ionization length ratio.

    作者:
    T Gyergyek, J Kovačič
    日期:
    2017-06-06

    A one-dimensional, two-fluid, steady state model is used for the analysis of ion temperature effects to the plasma-wall transition. In this paper, the model is solved for a finite ratio between the Debye and the ionization length, while in Part II [T. Gyergyek and J. Kovačič, Phys Plasmas 24, 063506 (2017)], the solutions for [Formula: see text] are presented. Ion temperature is treated as a given, independent parameter and it is included in the model as a boundary condition. It is shown that when the ion temperature larger than zero is selected, the ion flow velocity and the electric field at the boundary must be consistent with the selected ion temperature. A numerical procedure, how to determine such "consistent boundary conditions," is proposed, and a simple relation between the ion temperature and ion velocity at the boundary of the system is found. The effects of the ion temperature to the pre-sheath length, potential, ion temperature, and ion density drops in the pre-sheath and in the sheath are investigated. It is concluded that larger ion temperature results in a better shielding of the plasma from the wall. An attempt is made to include the ion heat flux into the model in its simplest form [Formula: see text], where [Formula: see text] is a constant heat conduction coefficient. It is shown that inclusion of such a term into the energy transfer equation introduces an additional ion heating mechanism into the system and the ion flow then becomes isothermal instead of adiabatic even in the sheath.

  8. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    8. Laser-plasmas in the relativistic-transparency regime: Science and applications.

    作者:
    Juan C Fernández, D Cort Gautier, Chengkung Huang, Sasikumar Palaniyappan, Brian J Albright, Woosuk Bang, Gilliss Dyer, Andrea Favalli, James F Hunter, Jacob Mendez, Markus Roth, Martyn Swinhoe, Paul A Bradley, Oliver Deppert, Michelle Espy, Katerina Falk, Nevzat Guler, Christopher Hamilton, Bjorn Manuel Hegelich, Daniela Henzlova, Kiril D Ianakiev, Metodi Iliev, Randall P Johnson, Annika Kleinschmidt, Adrian S Losko, Edward McCary, Michal Mocko, Ronald O Nelson, Rebecca Roycroft, Miguel A Santiago Cordoba, Victor A Schanz, Gabriel Schaumann, Derek W Schmidt, Adam Sefkow, Tsutomu Shimada, Terry N Taddeucci, Alexandra Tebartz, Sven C Vogel, Erik Vold, Glen A Wurden, Lin Yin
    日期:
    2017-05-30

    Laser-plasma interactions in the novel regime of relativistically induced transparency (RIT) have been harnessed to generate intense ion beams efficiently with average energies exceeding 10 MeV/nucleon (>100 MeV for protons) at "table-top" scales in experiments at the LANL Trident Laser. By further optimization of the laser and target, the RIT regime has been extended into a self-organized plasma mode. This mode yields an ion beam with much narrower energy spread while maintaining high ion energy and conversion efficiency. This mode involves self-generation of persistent high magnetic fields (∼10 T, according to particle-in-cell simulations of the experiments) at the rear-side of the plasma. These magnetic fields trap the laser-heated multi-MeV electrons, which generate a high localized electrostatic field (∼0.1 T V/m). After the laser exits the plasma, this electric field acts on a highly structured ion-beam distribution in phase space to reduce the energy spread, thus separating acceleration and energy-spread reduction. Thus, ion beams with narrow energy peaks at up to 18 MeV/nucleon are generated reproducibly with high efficiency (≈5%). The experimental demonstration has been done with 0.12 PW, high-contrast, 0.6 ps Gaussian 1.053 m laser pulses irradiating planar foils up to 250 nm thick at 2-8 × 10 W/cm. These ion beams with co-propagating electrons have been used on Trident for uniform volumetric isochoric heating to generate and study warm-dense matter at high densities. These beam plasmas have been directed also at a thick Ta disk to generate a directed, intense point-like Bremsstrahlung source of photons peaked at ∼2 MeV and used it for point projection radiography of thick high density objects. In addition, prior work on the intense neutron beam driven by an intense deuterium beam generated in the RIT regime has been extended. Neutron spectral control by means of a flexible converter-disk design has been demonstrated, and the neutron beam has been used for point-projection imaging of thick objects. The plans and prospects for further improvements and applications are also discussed.

  9. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    9. Verification of long wavelength electromagnetic modes with a gyrokinetic-fluid hybrid model in the XGC code.

    作者:
    Robert Hager, Jianying Lang, C S Chang, S Ku, Y Chen, S E Parker, M F Adams
    日期:
    2017-05-24

    As an alternative option to kinetic electrons, the gyrokinetic total-f particle-in-cell (PIC) code XGC1 has been extended to the MHD/fluid type electromagnetic regime by combining gyrokinetic PIC ions with massless drift-fluid electrons analogous to Chen and Parker [Phys. Plasmas , 441 (2001)]. Two representative long wavelength modes, shear Alfvén waves and resistive tearing modes, are verified in cylindrical and toroidal magnetic field geometries.

  10. JCR分区: Q2 CAS分区: B3 影响因子: 2.5

    10. The basis for cosmic ray feedback: Written on the wind.

    作者:
    Ellen G Zweibel
    日期:
    2017-05-24

    Star formation and supermassive black hole growth in galaxies appear to be self-limiting. The mechanisms for self-regulation are known as . Cosmic rays, the relativistic particle component of interstellar and intergalactic plasma, are among the agents of feedback. Because cosmic rays are virtually collisionless in the plasma environments of interest, their interaction with the ambient medium is primarily mediated by large scale magnetic fields and kinetic scale plasma waves. Because kinetic scales are much smaller than global scales, this interaction is most conveniently described by fluid models. In this paper, I discuss the kinetic theory and the classical theory of cosmic ray hydrodynamics (CCRH) which follows from assuming cosmic rays interact only with self-excited waves. I generalize CCRH to generalized cosmic ray hydrodynamics, which accommodates interactions with extrinsic turbulence, present examples of cosmic ray feedback, and assess where progress is needed.

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