{"title":"On turbulent magnetic reconnection: fast and slow mean steady-states","authors":"Sage Stanish, David MacTaggart","doi":"arxiv-2409.07346","DOIUrl":"https://doi.org/arxiv-2409.07346","url":null,"abstract":"We investigate a model of turbulent magnetic reconnection introduced by Yokoi\u0000and collaborators (Phys. Rev. Lett. 110, 255001) and show that the classic\u0000two-dimensional, steady-state Sweet-Parker and Petschek reconnection solutions\u0000are supported. We present evidence that these are the only two steady-state\u0000reconnection solutions, and we determine the criterion for their selection.\u0000Sweet-Parker reconnection occurs when there is no growth in turbulent energy,\u0000whereas Petschek reconnection occurs when the current density in the\u0000reconnecting current sheet is able to surpass a critical value, allowing for\u0000the growth of turbulent energy that creates the diffusion region. Further, we\u0000show that the Petschek solutions are self-similar, depending on the value of\u0000the turbulent time scale. The self-consistent development of Petschek\u0000reconnection through turbulence, within the model, is an example of fast and\u0000steady magnetic reconnection without an explicit need for the collisionless\u0000terms in an extended Ohm's law.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"24 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196021","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Numerical Investigations on Dilute Cold Plasma Potential and Electron Temperature","authors":"Shiying Cai, Chunpei Cai, Zhen Zhang","doi":"arxiv-2409.06758","DOIUrl":"https://doi.org/arxiv-2409.06758","url":null,"abstract":"Simulation results are presented to demonstrate electron temperature and\u0000electrical potential development in dilute and cold plasma development. The\u0000simulation method is a hybrid method which adopted fluid model for electrons\u0000due to their high mobility, while heavy ions and neutrals are modelled with the\u0000direct simulation Monte Carlo and Particle-In-Cell methods. The flows include\u0000steady, starting-up and shutting-down scenarios. The goal is to illustrate the\u0000exponential behaviors which were predicted in several recently developed\u0000formulas. Those formulas include many coefficients related with local\u0000properties, and they are difficult to determine. Hence, those trends can only\u0000efficiently demonstrate by numerical simulations which are more convenient than\u0000experimental measurements. The results confirm several facts. For steady plasma\u0000flows, the electron temperature and potential profiles are smooth, very likely,\u0000they can be approximated with exponential functions. For unsteady flows, the\u0000property developing trends in the shutting down or starting-up processes change\u0000monotonically. Further, at locations with large gradients, the property change\u0000trends are less ideal than those formulas. This is consistent with the\u0000assumptions with which those formulas were developed.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"9 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196024","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Theoretical Study of Inhomogeneity Effects on Three-Wave Parametric Instability: A WKBJ Approach","authors":"Taotao Zhou, Nong Xiang, Chunyun Gan, Tianyang Xia","doi":"arxiv-2409.06677","DOIUrl":"https://doi.org/arxiv-2409.06677","url":null,"abstract":"The mechanisms by which media inhomogeneity affects the three wave parametric\u0000instability (PI), including the wave number mismatch and the parameter\u0000gradients, are investigated using an approach based on the\u0000Wentzel-Kramers-Brillouin-Jeffreys (WKBJ) approximation. This approach\u0000transforms the coupling wave equations into an amplitude equation and\u0000iteratively solves its characteristic polynomials. By analyzing the solutions,\u0000we proposed that the wave number of the quasi-mode, a key term in the wave\u0000number mismatch of non-resonant type PI, should be a complex root of the\u0000quasi-mode's linear dispersion equation. Based on this, we derive a unified\u0000amplification factor formula that covers the resonant and non-resonant, the\u0000forward-scattered and backward-scattered types of PI. The impact of parameter\u0000gradients on the local spatial growth rate becomes significant when the\u0000inhomogeneity exceeds 10^{-3}. Considering parameter gradients extends our\u0000approach's validity to an inhomogeneity of about 10^{-2}. This approach holds\u0000promise for more specific PI modeling in the future.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"66 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196027","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Guillaume Bouchard, Arnaud Beck, Francesco Massimo, Arnd Specka
{"title":"Perfectly Matched Layer implementation for E-H fields and Complex Wave Envelope propagation in the Smilei PIC code","authors":"Guillaume Bouchard, Arnaud Beck, Francesco Massimo, Arnd Specka","doi":"arxiv-2409.06287","DOIUrl":"https://doi.org/arxiv-2409.06287","url":null,"abstract":"The design of absorbing boundary conditions (ABC) in a numerical simulation\u0000is a challenging task. In the best cases, spurious reflections remain for some\u0000angles of incidence or at certain wave lengths. In the worst, ABC are not even\u0000possible for the set of equations and/or numerical schemes used in the\u0000simulation and reflections can not be avoided at all. Perflectly Matched Layer\u0000(PML) are layers of absorbing medium which can be added at the simulation edges\u0000in order to significantly damp both outgoing and reflected waves, thus\u0000effectively playing the role of an ABC. They are able to absorb waves and\u0000prevent reflections for all angles and frequencies at a modest computational\u0000cost. It increases the simulation accuracy and negates the need of oversizing\u0000the simulation usually imposed by ABC and leading to a waste of computational\u0000resources and power. PML for finite-difference time-domain (FDTD) schemes in\u0000Particle-In-cell (PIC) codes are presented for both Maxwell's equations and,\u0000for the first time, the envelope wave equation. Being of the second order, the\u0000latter requires significant evolutions with respect to the former. It applies\u0000in particular to simulations of lasers propagating in plasmas using the reduced\u0000Complex Envelope model. The implementation is done in the open source code\u0000Smilei for both Cartesian and azimuthal modes (AM) decomposition geometries.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"62 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142225105","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Kink instability of flux ropes in partially-ionised plasmas","authors":"Giulia Murtas, Andrew Hillier, Ben Snow","doi":"arxiv-2409.06901","DOIUrl":"https://doi.org/arxiv-2409.06901","url":null,"abstract":"In the solar atmosphere, flux ropes are subject to current driven\u0000instabilities that are crucial in driving plasma eruptions, ejections and\u0000heating. A typical ideal magnetohydrodynamics (MHD) instability developing in\u0000flux ropes is the helical kink, which twists the flux rope axis. The growth of\u0000this instability can trigger magnetic reconnection, which can explain the\u0000formation of chromospheric jets and spicules, but its development has never\u0000been investigated in a partially-ionised plasma (PIP). Here we study the kink\u0000instability in PIP to understand how it develops in the solar chromosphere,\u0000where it is affected by charge-neutral interactions. Partial ionisation speeds\u0000up the onset of the non-linear phase of the instability, as the plasma $beta$\u0000of the isolated plasma is smaller than the total plasma $beta$ of the bulk.\u0000The distribution of the released magnetic energy changes in fully and\u0000partially-ionised plasmas, with a larger increase of internal energy associated\u0000to the PIP cases. The temperature in PIP increases faster also due to heating\u0000terms from the two-fluid dynamics. PIP effects trigger the kink instability on\u0000shorter time scales, which is reflected in a more explosive chromospheric flux\u0000rope dynamics. These results are crucial to understand the dynamics of\u0000small-scale chromospheric structures - mini-filament eruptions - that this far\u0000have been largely neglected but could significantly contribute to chromospheric\u0000heating and jet formation.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"179 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196025","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Enhancement of fusion reactivities using non-Maxwellian energy distributions","authors":"Ben I. Squarer, Carlo Presilla, Roberto Onofrio","doi":"arxiv-2409.05848","DOIUrl":"https://doi.org/arxiv-2409.05848","url":null,"abstract":"We discuss conditions for the enhancement of fusion reactivities arising from\u0000different choices of energy distribution functions for the reactants. The key\u0000element for potential gains in fusion reactivity is identified in the\u0000functional dependence of the tunnellng coefficient upon the energy, ensuring\u0000the existence of a finite range of temperatures for which reactivity of fusion\u0000processes is boosted with respect to the Maxwellian case. This is shown, using\u0000a convenient parameterization of the tunneling coefficient dependence upon the\u0000energy, analytically in the simplified case of a bimodal Maxwell-Boltzmann\u0000distribution, and numerically for kappa-distributions. We then consider\u0000tunneling potentials progressively better approximating fusion processes, and\u0000evaluate in each case the average reactivity in the case of\u0000kappa-distributions.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"69 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142195852","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
A. Baillod, E. J. Paul, G. Rawlinson, M. Haque, S. W. Freiberger, S. Thapa
{"title":"Integrating Novel Stellarator Single-Stage Optimization Algorithms to Design the Columbia Stellarator Experiment","authors":"A. Baillod, E. J. Paul, G. Rawlinson, M. Haque, S. W. Freiberger, S. Thapa","doi":"arxiv-2409.05261","DOIUrl":"https://doi.org/arxiv-2409.05261","url":null,"abstract":"The Columbia Stellarator eXperiment (CSX), currently being designed at\u0000Columbia University, aims to test theoretical predictions related to QA plasma\u0000behavior, and to pioneer the construction of an optimized stellarator using\u0000three-dimensional, non-insulated high-temperature superconducting (NI-HTS)\u0000coils. The magnetic configuration is generated by a combination of two circular\u0000planar poloidal field (PF) coils and two 3D-shaped interlinked (IL) coils, with\u0000the possibility to add windowpane coils to enhance shaping and experimental\u0000flexibility. The PF coils and vacuum vessel are repurposed from the former\u0000Columbia Non-Neutral Torus (CNT) experiment, while the IL coils will be\u0000custom-wound in-house using NI-HTS tapes. To obtain a plasma shape that meets\u0000the physics objectives with a limited number of coils, novel single-stage\u0000optimization techniques are employed, optimizing both the plasma and coils\u0000concurrently, in particular targeting a tight aspect ratio QA plasma and\u0000minimized strain on the HTS tape. Despite the increased complexity due to the\u0000expanded degrees of freedom, these methods successfully identify optimized\u0000plasma geometries that can be realized by coils meeting engineering\u0000specifications. This paper discusses the derivation of the constraints and\u0000objectives specific to CSX, and describe how two recently developed\u0000single-stage optimization methodologies are applied to the design of CSX. A set\u0000of selected configurations for CSX is then described in detail.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"11 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196030","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Jonathan Squire, Eliot Quataert, Philip F. Hopkins
{"title":"Rapid, strongly magnetized accretion in the zero-net-vertical-flux shearing box","authors":"Jonathan Squire, Eliot Quataert, Philip F. Hopkins","doi":"arxiv-2409.05467","DOIUrl":"https://doi.org/arxiv-2409.05467","url":null,"abstract":"We show that there exist two qualitatively different turbulent states of the\u0000zero-net-vertical-flux shearing box. The first, which has been studied in\u0000detail previously, is characterized by a weakly magnetized ($betasim50$)\u0000midplane with slow periodic reversals of the mean azimuthal field (dynamo\u0000cycles). The second (the \"low-$beta$ state\"), which is the main subject of\u0000this paper, is characterized by a strongly magnetized $betasim1$ midplane\u0000dominated by a coherent azimuthal field with much stronger turbulence and much\u0000larger accretion stress $alpha sim 1$. The low-$beta$ state is realized in\u0000simulations that begin with sufficiently strong azimuthal magnetic fields. The\u0000mean azimuthal field in the low-$beta$ state is quasi steady (no cycles) and\u0000is sustained by a dynamo mechanism that compensates for the continued loss of\u0000magnetic flux through the vertical boundaries; we attribute the dynamo to the\u0000combination of differential rotation and the Parker instability, although many\u0000of its details remain unclear. Vertical force balance in the low-$beta$ state\u0000is dominated by the mean magnetic pressure except at the midplane, where\u0000thermal pressure support is always important (this is true even when\u0000simulations are initialized at $betall1$, provided the thermal scale-height\u0000of the disk is well-resolved). The efficient angular momentum transport in the\u0000low-$beta$ state may resolve long-standing tension between predictions of\u0000magnetorotational turbulence (at high $beta$) and observations; likewise, the\u0000bifurcation in accretion states we find may be important for understanding the\u0000state transitions observed in dwarf novae, X-ray binaries, and changing-look\u0000AGN. We discuss directions for future work including the implications of our\u0000results for global accretion disk simulations.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"1 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142225086","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
D. López-Bruna, S. Denizeau, I. Predebon, A. La Rosa, C. Poggi, P. Agostinetti
{"title":"Faraday shield dissipation in the drivers of SPIDER based on electromagnetic 3D calculations","authors":"D. López-Bruna, S. Denizeau, I. Predebon, A. La Rosa, C. Poggi, P. Agostinetti","doi":"arxiv-2409.05821","DOIUrl":"https://doi.org/arxiv-2409.05821","url":null,"abstract":"SPIDER (Source for the Production of Ions of Deuterium Extracted from Rf\u0000plasma) is a full-scale prototype of the ITER NBI source. It is based on the\u0000concept of inductive coupling between radio-frequency current drive and plasma.\u0000Present three-dimensional (3D) electromagnetic calculations of stationary RF\u0000fields in SPIDER permit an evaluation of the power dissipation in its main\u0000constituents. Taking experimental plasma parameters as input, we concentrate on\u0000the power dissipation in the copper-made Faraday shield lateral wall (FSLW) of\u0000the source for discharges with and without a static magnetic filter field. In\u0000agreement with our previous results and a first comparison with calorimetry\u0000data from the FSLW cooling circuit, the FSLW cylinder alone absorbs around 50%\u0000of the available power for the studied plasma parameters. A hypothesized\u0000improvement of transport confinement may increase significantly the efficiency.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"23 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142196031","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Miguel Saavedra-Melo, Nelson Castro, Robert Marosi, Eva Rajo-Iglesias, Filippo Capolino
{"title":"Wideband Glide-Symmetric Double-Corrugated Gap-Waveguide Traveling-Wave Tube for Millimeter Waves","authors":"Miguel Saavedra-Melo, Nelson Castro, Robert Marosi, Eva Rajo-Iglesias, Filippo Capolino","doi":"arxiv-2409.05238","DOIUrl":"https://doi.org/arxiv-2409.05238","url":null,"abstract":"We explore the use of glide symmetry (GS) and electromagnetic bandgap (EBG)\u0000technology in a glide-symmetric double corrugated gap waveguide (GSDC-GW) slow\u0000wave structure (SWS) for traveling wave tube (TWT) applications. Notably, this\u0000GS structure provides the advantage of wide-band operation and the EBG\u0000eliminates the need for a conductive connection between the top and bottom\u0000waveguide plates. The TWT performance is evaluated via particle-in-cell\u0000simulations that reveal a 3-dB bandwidth of approximately 12 GHz spanning from\u000054.5 GHz to 66.3 GHz, accompanied by a maximum gain of 23 dB. Because of GS,\u0000the backward wave in the first spatial harmonic is not longitudinally\u0000polarized, leading to a low risk of backward wave oscillations in the TWT. This\u0000work places the GSDC-EBG structure within the arena of potential SWS topologies\u0000for TWTs operating under similar conditions.","PeriodicalId":501274,"journal":{"name":"arXiv - PHYS - Plasma Physics","volume":"27 1","pages":""},"PeriodicalIF":0.0,"publicationDate":"2024-09-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142225058","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}