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Issue Information: Contrib. Plasma Phys. 06/2025 发行信息:投稿。等离子体物理。6/2025
IF 1.3 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-07-08 DOI: 10.1002/ctpp.202590012
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引用次数: 0
Predicting the Uniform Electron Gas Stopping Power at Moderate and Strong Coupling 中强耦合下均匀电子阻气功率的预测
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-07-02 DOI: 10.1002/ctpp.70026
Saule A. Syzganbayeva, Alexey V. Filinov, Jesús Ara, Assel B. Ashikbayeva, Abdiadil Askaruly, Lazzat T. Yerimbetova, Manuel D. Barriga-Carrasco, Yuriy V. Arkhipov, Igor M. Tkachenko

This paper presents a detailed study of the stopping power of a homogeneous electron gas in moderate and strong coupling regimes using the self-consistent version of the method of moments as the key theoretical approach capable of expressing the dynamic characteristics of the system in terms of the static ones, which are the moments. We develop a robust framework that relies on nine sum rules and other exact relationships to analyze electron–electron interactions and their impact on energy loss processes. We derive an expression for the stopping power that takes into account both quantum statistical effects and electron correlation phenomena. Our results demonstrate significant deviations from classical stopping power predictions, especially under the strong coupling conditions, where electron dynamics are highly dependent on the collective behavior. This work not only advances the theoretical understanding of the homogeneous electron gas but also has implications for practical applications in fields such as plasma physics and materials science.

本文采用矩量法的自洽版本作为关键的理论方法,详细研究了均质电子气体在中等和强耦合状态下的停止能力,该方法能够用静态特性(即矩量)来表达系统的动态特性。我们开发了一个强大的框架,它依赖于九和规则和其他精确的关系来分析电子-电子相互作用及其对能量损失过程的影响。我们推导了一个同时考虑量子统计效应和电子相关现象的停止功率表达式。我们的结果显示了与经典停止功率预测的显著偏差,特别是在强耦合条件下,电子动力学高度依赖于集体行为。这项工作不仅推进了对均相电子气体的理论认识,而且对等离子体物理和材料科学等领域的实际应用也具有重要意义。
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引用次数: 0
Demarcating the Classical and Quantum Approaches for the Coulomb Logarithm in Plasmas 等离子体中库仑对数的经典方法和量子方法的区分
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-07-01 DOI: 10.1002/ctpp.70033
S. K. Kodanova, T. S. Ramazanov, M. K. Issanova

The Coulomb logarithm often enters various plasma models and simulation methods for computing the transport and relaxation properties of plasmas. Traditionally, a classical pair collision picture was used to calculate the Coulomb logarithm for different plasma parameters. With the recent emergence of the high interest in dense plasmas with partially degenerate electrons, new approaches have been developed to treat electron-ion collisions in a quantum-mechanical way. In this context, gaining a deeper physical understanding of the criteria for the applicability of classical plasma models is crucial. We have analyzed the Coulomb logarithm describing the electron-ion collisions in hydrogen plasmas in a wide range of temperatures and densities relevant to inertial confinement fusion experiments. The electron-ion collision cross-sections were computed using both quantum and classical scattering theories. We found that the classical description of the electron-ion scattering in plasmas and related plasma models is applicable if the de Broglie wavelength of electrons is smaller than the ion charge screening length in plasmas. Additionally, we show that the quantum first-order Born approximation for describing the electron-ion collision is accurate only in the regime where classical scattering theory is accurate.

库仑对数经常进入各种等离子体模型和模拟方法中,用于计算等离子体的输运和弛豫特性。传统上,采用经典的对碰撞图来计算不同等离子体参数下的库仑对数。随着近年来人们对具有部分简并电子的致密等离子体的高度兴趣的出现,用量子力学的方法来处理电子-离子碰撞的新方法已经发展起来。在这种情况下,获得对经典等离子体模型适用性标准的更深入的物理理解是至关重要的。我们分析了在与惯性约束聚变实验相关的大范围温度和密度下氢等离子体中电子-离子碰撞的库仑对数。利用量子散射理论和经典散射理论计算了电子-离子碰撞截面。我们发现,当电子的德布罗意波长小于等离子体中的离子电荷屏蔽长度时,等离子体中电子-离子散射的经典描述和相关的等离子体模型是适用的。此外,我们证明描述电子-离子碰撞的量子一阶玻恩近似仅在经典散射理论准确的区域是准确的。
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引用次数: 0
Cover Picture: Contrib. Plasma Phys. 05/2025 封面图片:投稿。等离子体物理。05/2025
IF 1.3 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-06-18 DOI: 10.1002/ctpp.202590009

Spatial distribution of particles hitting the collector probes based on different simulations for the DIII-Dcase: (a) 40 million, (b) 80 million, (c) 160 million. Fig.18 of the paper by Dhyanjyoti D. Nath et al. https://doi.org/10.1002/ctpp.202400073

基于DIII-Dcase不同模拟的粒子撞击收集器探针的空间分布:(a) 4000万,(b) 8000万,(c) 1.6亿。Dhyanjyoti D. Nath等人的论文图18 https://doi.org/10.1002/ctpp.202400073
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引用次数: 0
Issue Information: Contrib. Plasma Phys. 05/2025 发行信息:投稿。等离子体物理。05/2025
IF 1.3 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-06-18 DOI: 10.1002/ctpp.202590010
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引用次数: 0
Charged Particle Transport in Magnetic Turbulence 磁湍流中的带电粒子输运
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-06-15 DOI: 10.1002/ctpp.70018
Yasuhiro Kuramitsu, Tohru Hada

We discuss charged particle transport in a turbulent magnetic field. The pitch angle diffusion is essential to the transport processes of energetic particles in real and momentum spaces. We integrate particle trajectories in time under the influence of the turbulent magnetic field given as a superposition of parallel-propagating magnetohydrodynamic waves (“slab-turbulence”). As in the standard theory for cosmic ray transports, the small wave amplitude and the random phase approximation are the fundamental assumptions of the quasi-linear theory. In the presence of large amplitude waves, our numerical study shows the anomalous pitch angle diffusion of the energetic particles. In the presence of waves with strong phase correlation, where the MHD turbulence is represented as intermittent wave packets, the particles are transported in the momentum space due to the mirror reflections rather than the pitch angle diffusion. The particle motions are mostly ballistic and occasionally reflected by the intermittent wave packets; thus, the spatial transport of the energetic particles can be super-diffusive in the presence of large amplitude MHD waves with strong phase correlation.

我们讨论了带电粒子在湍流磁场中的输运。俯仰角扩散对高能粒子在实空间和动量空间中的输运过程至关重要。我们在紊流磁场的影响下对粒子的时间轨迹进行积分,紊流磁场是平行传播的磁流体动力波(“板湍流”)的叠加。与宇宙射线传输的标准理论一样,小波幅和随机相位近似是准线性理论的基本假设。在大振幅波存在的情况下,我们的数值研究显示了高能粒子的异常俯仰角扩散。在具有强相位相关性的波的存在下,MHD湍流被表示为间歇波包,粒子在动量空间中由于镜像反射而不是俯仰角扩散而传输。粒子运动以弹道运动为主,偶有间歇波包反射;因此,在具有强相位相关性的大振幅MHD波存在下,高能粒子的空间输运可能是超扩散的。
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引用次数: 0
Numerical Modeling of Isochoric Heating Experiments Using the Troll Code in the Warm Dense Matter Regime 热致密物质区等时程加热实验的Troll代码数值模拟
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-06-12 DOI: 10.1002/ctpp.70030
Sébastien Rassou, Marie Bonneau, Christophe Rousseaux, Xavier Vaisseau, Witold Cayzac, Adrien Denoeud, Frédéric Perez, Tom Beaumont, Morris Demoulins, Jean-Christophe Pain

Experiments of isochoric heating by protons of solid material were recently performed at LULI laser facilities. In these experiments, protons, produced from target normal sheath acceleration (TNSA) of Au foil with the PICO2000 laser, deposit their energy into an aluminum or copper foil initially at room temperature and solid density. The heated material reaches the warm dense matter regime with temperature in the rear face of the material between 1 and 5 eV. The temperature is inferred by streaked optical pyrometry and the proton beam is characterized by Thomson parabola. The high-energy protons produced by TNSA are modeled to deduce the initial proton distribution before the slowing down in the target. Hydrodynamic radiative simulations were next performed using the Troll code in multidimensional geometry. In the Troll code, the heating of protons is modeled with a Monte Carlo transport module of charged particles and the calculation of the energy deposited by the protons in the matter is performed using stopping power formulas like Srim functions. The results of simulations with the Troll code are compared with the experimental results. An acceptable agreement between experiment and simulation is found for the temperature at the rear of the material using Sesame equation of state and Srim stopping power for protons in aluminum.

最近在LULI激光设备上进行了固体材料的质子等共时加热实验。在这些实验中,用PICO2000激光从金箔的目标正常鞘层加速(TNSA)产生的质子,在室温和固体密度下最初将其能量沉积到铝或铜箔中。加热后的材料达到热致密物质状态,材料背面的温度在1到5 eV之间。温度由条纹光学热分析法推断,质子束用汤姆逊抛物线表征。对TNSA产生的高能质子进行了模拟,推导出了靶内减速前的初始质子分布。然后利用Troll代码在多维几何中进行水动力辐射模拟。在Troll代码中,质子的加热是用带电粒子的蒙特卡罗输运模块来模拟的,而质子在物质中沉积的能量的计算则是使用像Srim函数这样的停止功率公式来执行的。利用Troll代码对仿真结果与实验结果进行了比较。利用芝麻状态方程和铝中质子的Srim停止功率对材料后部的温度进行了实验和模拟,得到了较好的一致性。
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引用次数: 0
Optimization of Ion Acceleration by Irradiating Large-Area Suspended Graphene With a Picosecond Laser 皮秒激光照射大面积悬浮石墨烯优化离子加速
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-05-28 DOI: 10.1002/ctpp.70016
Naoya Tamaki, Takumi Minami, Soichiro Suzuki, Yasuhiro Kuramitsu

By irradiating an ultra-thin graphene target, large-area suspended graphene (LSG) with a picosecond and moderate-intensity laser, protons with energies exceeding 100 MeV have been achieved. However, the optimal conditions for ion acceleration in such an atomic-thin target regime using a picosecond intense laser remain unclear. By performing particle-in-cell (PIC) simulations, we discuss optimum conditions to realize energy frontier of laser-driven ion acceleration. Parameter scans over LSG thickness and laser F$$ F $$-number reveals the optimal conditions under which proton energies exceed 500 MeV. This can be realized with the upgraded laser focus of the LFEX in the future.

利用皮秒中等强度激光照射超薄石墨烯靶材大面积悬浮石墨烯(LSG),获得了能量超过100 MeV的质子。然而,在这种原子薄的靶区使用皮秒强激光加速离子的最佳条件仍不清楚。通过粒子池(PIC)模拟,讨论了实现激光驱动离子加速能量前沿的最佳条件。对LSG厚度和激光F $$ F $$ -数的参数扫描揭示了质子能量超过500 MeV的最佳条件。这可以通过未来LFEX的激光聚焦升级来实现。
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引用次数: 0
Electron Density Structure Measurements With Scattered Intense Laser Beam 用散射强激光束测量电子密度结构
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-05-23 DOI: 10.1002/ctpp.70020
K. Sakai, K. Himeno, S. J. Tanaka, T. Asai, T. Minami, Y. Abe, F. Nikaido, K. Kuramoto, M. Kanasaki, H. Kiriyama, A. Kon, K. Kondo, N. Nakanii, W. Y. Woon, C. M. Chu, K. T. Wu, C. S. Jao, Y. L. Liu, T. A. Pikuz, H. Kohri, A. O. Tokiyasu, S. Isayama, H. S. Kumar, K. Tomita, Y. Fukuda, Y. Kuramitsu

Short-pulse intense lasers have the potential to model extreme astrophysical environments in laboratories. Although there are diagnostics for energetic electrons and ions resulting from laser-plasma interactions, the diagnostics to measure velocity distribution functions at the interaction region of the laser and plasma are limited. We have been developing the diagnostics of the interaction between the intense laser and plasma using scattered intense laser. We performed experiments to measure electron density by observing the spatial distributions and the ratio of horizontal to vertical polarization components of the scattered laser beam using optical imaging. The observed ratio of polarization components is consistent with the drive laser beam, indicating the observed light originates from the drive laser. Imaging of the scattered light shows the structure of electron density, the zero moment of the electron velocity distribution function, interacting with the intense laser. We observed the change of structure due to the laser pre-pulse that destroys the target before the arrival of the main pulse.

短脉冲强激光有可能在实验室中模拟极端的天体物理环境。虽然对激光与等离子体相互作用产生的高能电子和离子进行了诊断,但测量激光与等离子体相互作用区域的速度分布函数的诊断是有限的。我们一直在利用散射强激光发展强激光与等离子体相互作用的诊断。利用光学成像技术,通过观察散射激光束的空间分布和水平偏振分量与垂直偏振分量的比值,进行了测量电子密度的实验。观测到的偏振分量的比值与驱动激光束的比值一致,说明观测到的光来源于驱动激光。散射光成像显示了与强激光相互作用的电子密度结构,即电子速度分布函数的零矩。我们观察到由于激光预脉冲在主脉冲到达之前破坏了目标而引起的结构变化。
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引用次数: 0
Non-Markovian Quantum Kinetic Simulations of Uniform Dense Plasmas: Mitigating the Aliasing Problem 均匀致密等离子体的非马尔可夫量子动力学模拟:减轻混叠问题
IF 1.5 4区 物理与天体物理 Q3 PHYSICS, FLUIDS & PLASMAS Pub Date : 2025-05-23 DOI: 10.1002/ctpp.70022
C. Makait, M. Bonitz

Dense quantum plasmas out of equilibrium are successfully modeled using quantum kinetic equations, such as the quantum Boltzmann, Landau, or Balescu–Lenard equation. However, these equations do not properly take into account correlation effects, which require the use of generalized non-Markovian kinetic equations. While the latter have been successful for lattice models, applications to continuous systems such as plasmas are severely hampered by aliasing effects. Here we present a strategy for suppressing aliasing and making applications of non-Markovian quantum kinetic equations to plasmas possible.

利用量子动力学方程,如量子玻尔兹曼方程、朗道方程或Balescu-Lenard方程,成功地模拟了脱离平衡态的致密量子等离子体。然而,这些方程没有适当地考虑到相关效应,这需要使用广义非马尔可夫动力学方程。虽然后者在晶格模型中取得了成功,但在等离子体等连续系统中的应用受到混叠效应的严重阻碍。本文提出了一种抑制混叠的策略,使非马尔可夫量子动力学方程在等离子体中的应用成为可能。
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引用次数: 0
期刊
Contributions to Plasma Physics
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