Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session BO4: HEDP Laboratory Astrophysics and Shocks |
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Chair: Will Fox, PPPL Room: OCC B110-112 |
Monday, November 5, 2018 9:30AM - 9:42AM |
BO4.00001: Charged particle transport in laser-driven magnetized turbulence: understanding the intergalactic voyage of ultra-high energy cosmic rays Petros Tzeferacos, Laura E Chen, Archie Bott, Alexandra Rigby, Anthony R. Bell, Robert Bingham, Joe Katz, Michel Koenig, Chikang Li, Richard David Petrasso, Hye-Sook Park, J. Steven Ross, Dongsu Ryu, Dmitri D Ryutov, Thomas G White, Brian Reville, James Matthews, Jena Meinecke, Francesco Miniati, Ellen Gould Zweibel, Subir Sarkar, Alexander A Schekochihin, Dustin H Froula, Don Q Lamb, Gianluca Gregori How charged particles and turbulent magnetic fields interact is key to understanding the journey of cosmic rays through space. In this talk we report on numerical simulations and laser-driven experiments at the OMEGA Laser Facility that measure the propagation of energetic particles through random magnetic fields in a turbulent plasma. We characterize their angular diffusion and recover their mean free path and associated diffusion coefficients. The OMEGA experiments we present constitute the first laboratory probe of particle diffusion through magnetized turbulence in the absence of a mean background field and complement laboratory studies of energetic particle propagation in diffuse plasmas, where there is a strong guide field. The experiments emulate the propagation of ultra-high energy cosmic rays through the intergalactic medium, critical for interpreting anisotropies in their arrival direction and for constraining the distance of their sources |
Monday, November 5, 2018 9:42AM - 9:54AM |
BO4.00002: Magnetised turbulence in high-energy-density pulsed-power-driven experiments Jack Davies Hare, Sergey V Lebedev, Nuno F Loureiro, Andrea Ciardi, Samuel Eardley, Jack WD Halliday, George Rowland, Daniel Russell, Roland A Smith, Nicholas Stuart, Francisco Suzuki-Vidal, Lee Suttle, Eleanor Tubman Plasmas in astrophysical environments are generally turbulent, and this turbulence is a key driver of many important phenomena, including the magnetic dynamo. The study of astrophysically relevant turbulence in the laboratory poses two challenges - accessing high Reynolds numbers on laboratory length scales, and reliably diagnosing the fundamentally three-dimensional nature of the turbulence. We present experimental results from a new pulsed-power-driven platform, in which magnetised supersonic carbon flows converge inside a cylindrical wire array to produce a column of turbulent plasma.This column is confined for much longer than the hydrodynamic time scales by continuous inflows of plasma from the wires. We observe density perturbations over a broad range of length-scales using laser shadowgraphy. The magnetic fields advected by the flows are dynamically and energetically significant, allowing us to access an interesting regime of magnetised turbulence. We characterise this plasma using a suite of spatially and temporally resolved diagnostics, including ultra high speed imaging, laser shadowgraphy, interferometry, Thomson scattering and Faraday rotation imaging. |
Monday, November 5, 2018 9:54AM - 10:06AM |
BO4.00003: The interaction of a magnetized plasma flow with strongly magnetized bodies in HEDP experiments Lee Suttle, Chung Cheung, Putri Rusli, Catalina Garcia, Sergey V Lebedev, Jeremy Chittenden, Jonathan WD Halliday, Jack D Hare, Daniel Russell, Francisco Suzuki-Vidal, Eleanor Tubman Interactions of fast-streaming, magnetized plasmas can result in a wide range of fundamental plasma physics processes such as the formation of MHD shocks, magnetic turbulence, reconnection and wave-particle interactions. We present experiments where a plasma flow generated by the ablation of a pulsed-power driven wire array interacts with strongly magnetized obstacles. The plasma flow is super-Alfvénic (MA=2) and contains an embedded magnetic field (B~2T, ReM~100). The magnetization and magnetic field geometry of the obstacles can be controlled to study a range of interaction types and topologies. The choice of wire material also allows a variation of the collisionality of the plasma, as well as the strength of radiative cooling. The detailed structure of the interactions is measured using Thomson scattering, laser interferometry and Faraday rotation diagnostics, providing measurements of the flow velocity, plasma temperature, electron density and magnetic field distributions of the plasma. |
Monday, November 5, 2018 10:06AM - 10:18AM |
BO4.00004: Modeling of Laser-Generated Plasmas in a MG Magnetic Field L. S. Leal, A. V. Maximov, A. B. Sefkow, R. Betti, V. V. Ivanov Experiments coupling a plasma generated by a laser pulse with fields generated by pulsed power have shown that localized plasma structures (disk or ring) are present long after the pulse has ended.[1] We model the effects of coupling a pulse of intensity ( ~1015 W/cm2) with a field in the azimuthal direction of ~4 MG generated by axial current in a rod in 2 spatial dimensions. We are able to see localized structures that exist in the presence of the azimuthal field that are not seen when no field (current) is present. These localized plasma structures resembling a disk continue to expand in both the axial and radial directions. The pulse initially expels the field from the plasma; however, later in time the field generated in the localized structure reaches the same order of magnitude as the initial field. We also investigate how the parameters β (beta) and χ (Hall) vary as the localized structure evolves in time. [1] V. V. Ivanov et al., Plasma Phys. Control. Fusion 59, 085008 (2017). |
Monday, November 5, 2018 10:18AM - 10:30AM |
BO4.00005: Experimental investigation of pre-magnetization effects on laser-plasma dynamo processes. Archie F. A. Bott, Petros Tzeferacos, Laura E. Chen, Charlotte A. J. Palmer, Anthony R. Bell, Robert Bingham, Andrew Birkel, John Foster, Carlo Graziani, Joe Katz, Chikang Li, James Matthews, Fredrick H. Seguin, Jena Meinecke, Hye-Sook Park, James Ross, Brian Reville, Subir Sarkar, Dustin H. Froula, Alex A. Schekochihin, Don Q. Lamb, Gianluca Gregori It has recently been demonstrated experimentally on the OMEGA Laser Facility that a turbulent plasma created by the collision of two destabilized (but initially unmagnetized) plasma jets is capable of generating strong stochastic magnetic fields via the small-scale turbulent dynamo mechanism, provided the plasma's magnetic Reynolds number is sufficiently high (Tzeferacos et. al., Nat. Comm., vol. 9, 2018, 591). In this talk, we compare such a plasma with one arising from two pre-magnetized plasma jets, whose creation is identical save for the presence of a 10 T external magnetic field imposed by a pulsed magnetic field generator. We investigate differences between the two turbulent systems using Thomson scattering diagnostics, self-emitted X-ray imaging and proton radiography. While the Thomson scattering spectra are broadly similar between the magnetized and unmagnetized interactions, the proton radiographs are qualitatively different. In addition, the self-emitted X-rays in the magnetized interaction show a greater variation in relative magnitude between adjacent structures, a possible indication that the external field is capable of significantly altering the dynamics of the turbulent plasma despite only possessing a finite fraction of the initial plasma-jet kinetic energy. |
Monday, November 5, 2018 10:30AM - 10:42AM |
BO4.00006: Proton radiography of a highly asymmetric laser-driven magnetic reconnection geometry Paul T. Campbell, Gennady Fiksel, Chad Mileham, Philip M. Nilson, Alexander G. R. Thomas, Louise Willingale, Karl Krushelnick In experiments performed at the OMEGA EP laser facility at the Laboratory for Laser Energetics, the typical laser-driven magnetic reconnection geometry was adapted such that one high intensity pulse (I ≈ 1019 Wcm-2) was focused alongside a moderate intensity UV long pulse (I ≈ 1014 Wcm-2) on foil targets. First, the long pulse ablates a region of the target and misaligned temperature and density gradients in the plasma plume generate an azimuthal magnetic field via the Biermann battery mechanism. After the Biermann field develops, the high intensity pulse arrives on target and produces a relativistic, highly magnetized plasma (σ = B2/μ0nemec2 ≥ 1) which sweeps across the target surface with velocities near the speed of light. Proton radiography captures the evolution of the strong, impulsive magnetic field generated by the high intensity pulse and its interaction with the relatively slowly evolving Biermann battery fields. Quantitative measurements of the magnetic field dynamics will be presented, as well as 2D and 3D particle-in-cell simulation results. |
Monday, November 5, 2018 10:42AM - 10:54AM |
BO4.00007: Progress on astrophysical collisionless shock experiments on Omega and NIF Hye-Sook Park, Drew P Higginson, Bruce Allen Remington, Hans Rinderknecht, James Ross, Dmitri D Ryutov, George F Swadling, Scott Wilks, Frederico Fiuza, Anna Grassi, Anatoly Spitkovsky, Richard David Petrasso, Chikang Li We report the latest experimental progress on our laboratory experiments using the Omega and NIF lasers to investigate the dynamics of high Mach number collisionless shock formation in two interpenetrating plasma streams. It is believed that in astrophysical environments such shocks generate and amplified magnetic fields and accelerate cosmic rays. Counterstreaming plasma flows generated by laser ablation have been probed on the Omega laser using proton radiography, showing the formation, growth, and merger of filamentary magnetic field structures associated with the Weibel instability in a collisionless regime [1]. Recently, higher-energy experiments using the NIF laser showed enhanced heating when the flow interaction transited from collisional to collisionless flows [2]. The latest experiments on NIF considerably reduced collisionality and increased interaction volume. Significantly enhanced neutron production and high energy electrons were observed. We will present these recent experimental results. [1] C. M. Huntington, et al., Nature Physics, 11, 173 (2015); [2] J. S. Ross et al., Phys. Rev. Lett., 118, 185003 (2017). |
Monday, November 5, 2018 10:54AM - 11:06AM |
BO4.00008: Collisionless shock formation and particle acceleration in conditions relevant for NIF experiments Anna Grassi, Drew P Higginson, Hans Rinderknecht, George F Swadling, Dmitri D Ryutov, Hye-Sook Park, Frederico Fiuza Collisionless shocks are ubiquitous in the Universe and play an important role in the slow down of plasma flows, magnetic field generation/amplification, and particle acceleration. Depending on the plasma conditions, different plasma processes are believed to mediate shock formation and particle injection, however, these are not yet fully understood. Kinetic plasma simulations and high-energy-density (HED) laser-plasma experiments can help probe different plasma conditions and identify the dominant processes. We will present recent particle-in-cell (PIC) simulations of counter-streaming plasma flows for conditions relevant to ongoing collisionless shock experiments at the National Ignition Facility (NIF). The simulations take into account the time-dependent density and velocity profiles of the flows, that are inferred from hydrodynamical simulations. We will discuss the signatures of shock formation, the onset of particle acceleration, and the role of collisional effects. Finally, we will compare the simulations with the some of the first experimental results from NIF. |
Monday, November 5, 2018 11:06AM - 11:18AM |
BO4.00009: Laboratory Observations of Electron Heating in High-Mach-Number Collisionless Shocks Derek Schaeffer, William Fox, Russell Follett, Gennady Fiksel, Jackson Matteucci, Amitava Bhattacharjee, Kai Germaschewski Collisionless shocks are ubiquitous throughout the heliosphere, from planetary bow shocks to interplanetary shocks driven by coronal mass ejections to the termination shock at the edge of solar system. How these collisionless shocks heat plasmas remains a key heliophysics science question. Theory predicts the total plasma temperature in regions far from the shock interface, but despite decades of observations and numerical simulations, there remains no clear understanding on how energy is partitioned across the shock itself. Recent experiments [1] demonstrated the laboratory generation of high-Mach-number, magnetized collisionless shocks through the interaction of a laser-driven piston plasma with a pre-formed magnetized ambient plasma, opening up a new regime of laboratory space physics. We present new experiments utilizing this platform that measure electron heating through high-Mach-number collisionless shocks. The temperatures are diagnosed with temporally-resolved Thomson scattering, and the results are compared to both particle-in-cell simulations and satellite observations of electron heating in the Earth's bow shock. [1] Schaeffer et al., Phys. Rev. Lett. 119, 025001 (2017) |
Monday, November 5, 2018 11:18AM - 11:30AM |
BO4.00010: Magnetized Bow Shocks on OMEGA: Comparing Experimental Observations with Theory and Simulation Joseph M Levesque, Carolyn C Kuranz, Rachel Young, William J Gray, Matthew Trantham, Andy Liao, Patrick Hartigan, Sallee Klein, Gennady Fiksel, Mario Manuel, Joseph Katz, Chikang Li, Andrew Birkel Experiments studying magnetized bow shocks at the OMEGA laser facility have yielded quantitative measurements of plasma parameters across a shock front using the spatially resolved optical Imaging Thomson Scattering diagnostic (ITS). The bow shock system consists of a relatively slow, low-density plasma flow impinging on the azimuthal magnetic field imposed by a current-carrying wire. We infer electron number density and temperature from the Thomson scattered spectra, from which we determine the shock standoff distance. The data collected for two different levels of current in the wire suggests that the shock exists farther from the wire for stronger magnetic fields. We compare the inferred shock standoff distances to analytical models and to MHD simulations using the FLASH code. |
Monday, November 5, 2018 11:30AM - 11:42AM |
BO4.00011: Oblique shocks formed in magnetized plasma flows Eleanor R Tubman, Sergey V Lebedev, Guy C Burdiak, Lee Suttle, Daniel Russell, Jack D Hare, Simon N Bland, Samuel Eardley, Jonathan WD Halliday, George Rowland, Roland A Smith, Nicholas Stuart, Francisco Suzuki-Vidal We present experiments investigating the interaction of magnetized supersonic plasma flows with different conducting obstacles. Using the MAGPIE facility at Imperial College, London we are able to drive plasma flows from the ablation of inverse wire arrays. The flows are supersonic and super-Alfvenic (vflow ∼70 km/s, MA ∼2.5, M∼5) with frozen in magnetic fields of ∼1-2 T [1]. Wire grids placed into the flow, orientated parallel or perpendicular to the advected B-fields are used to control the magnetic field magnitude in the post-grid flow. This then affects the structure of both a network of oblique shocks [2,3] formed after the grid as well as the bow shock [4] formed at an additional, compact obstacle placed further downstream in the flow. Spatially and temporally resolved measurements, obtained using Thomson scattering, laser interferometry, shadowgraphy and Faraday rotation polarimetry, will be presented and discussed. [1] A. J. Harvey-Thompson et al., PoP 16 (2009) [2] G. F. Swadling et al., PoP 20 (2013) [3] S. V. Lebedev et al., PoP 21 (2014) [4] G. C. Burdiak et al., PoP 24 (2017) |
Monday, November 5, 2018 11:42AM - 11:54AM |
BO4.00012: Study of self-generated magnetic field at the front of a strong shock in helium Rui Hua, Joohwan Kim, Mark Sherlock, Mathieu Bailly-Grandvaux, Farhat N Beg, Christopher S McGuffey, Scott Wilks, Frank R Graziani, Yuan Ping We report for the first time a measurement of the magnetic field at the front of a Mach 6 shock propagating in a low-density helium gas system. In the experiments, strong shock waves were generated using two long pulse beams of 1 kJ total energy in 0.5 ns square pulse from OMEGA EP laser system. The generated shock was propagating under a quasi-planar geometry and diagnosed by broadband proton radiography. TNSA protons are produced by a 10 ps, 400 J short pulse interacting with a copper foil. Shock conditions such as temperature and density are constrained by X-ray spectrometry measurements to be ~ 140 eV and ~ 1.5 mg/cc respectively. The existence of the magnetic field is confirmed by point projection proton radiography from different angles. Calculations of the field strength ~ 5 to 7 T and thickness ~ 120 μm are also achieved by quantitative analysis of the proton radiography data. The measured self-generated magnetic field was further confirmed using the hybrid particle-in-cell code. |
Monday, November 5, 2018 11:54AM - 12:06PM |
BO4.00013: Design of radiative shocktube experiments with X-ray Thomson scattering measurements on the National Ignition Facility Kevin Hao Ma, Heath Joseph LeFevre, Patrick X Belancourt, M. J. MacDonald, Tilo Doeppner, Channing M Huntington, Carolyn C Kuranz, Eric Johnsen
Previous experiments at the National Ignition Facility (NIF) studied the effect of high-energy fluxes from radiation and electron heat conduction on shock-driven hydrodynamic instability perturbation growth. Experimental results exhibited reduced growth in the high-energy flux case compared to experiments with negligible energy fluxes [1]. It is hypothesized this reduced growth is due to ablative stabilization from radiative and thermal conduction energy fluxes in the hot, shocked foam. We plan to implement X-Ray Thomson Scattering (XRTS) in the radiative shock tube platform to measure electron temperatures in the shocked foam. We present simulations in CRASH, an Eulerian radiation hydrodynamics code, which predict shock speeds, electron temperatures, and effective ionizations in SiO2 and carbon foams. In addition, we assess plasma parameters in the measurement region and give initial estimations of the XRTS spectra. Shot days for this experiment are scheduled on the NIF in 2019 and 2020.[1] C.C. Kuranz, H.-S. Park et. al, Nat. Commun. 9, 1564 (2008) |
Monday, November 5, 2018 12:06PM - 12:18PM |
BO4.00014: Design of a pulsed-power magnetized plasma flow experiment for the study of star formation and astrophysical bow shocks Raul F Melean, Rachel Young, Sallee Klein, Paul C Campbell, Nicholas M Jordan, Ryan D McBride, Carolyn C Kuranz We present the design of two laboratory-astrophysics experiments with the goal of translating research performed at a major (several kJ) laser facility into the pulsed-power laboratory at the Michigan Accelerator for Inductive Z-Pinch Experiments (MAIZE). The experiments are designed to explore the interactions of magnetized plasma flows in astrophysical bow shocks and accretion shocks found in star formation, with a focus in the structure and development of shock instabilities. To accomplish this, we will be generating magnetized plasma flows via pulsed-power in the Linear Transformer Drive (LTD) at the University of Michigan, by ablating aluminum wire arrays with currents of up to 1 Mega- Amp. We have designed two different array geometries: a cylindrical wire array that will be used to study bow shock interactions against a variety of magnetized targets (conducting wires, electromagnets and permanent magnets), and a conical array that will drive a plasma jet into a solid target for the study accretion shocks. |
Monday, November 5, 2018 12:18PM - 12:30PM |
BO4.00015: Diagnostic signatures of magnetized collisionless shocks in laboratory experiments Zhenyu Wang, Anatoly Spitkovsky, Channing M Huntington, Hye-Sook Park, Steven Ross, Frederico Fiuza, Dmitri D Ryutov, Bradley Pollock, Scott Wilks Magnetized collisionless shocks commonly occur in the heliosphere and astrophysics, and have recently become the subject of laboratory investigations at HED facilities. We describe the modeling and interpretation of a campaign of laser experiments designed to generate high Mach number magnetized collisionless shocks on OMEGA-EP. In the experiment, a laser-produced high velocity plasma collides with a magnetized, pre-ablated plasma. Proton radiography shows a moving region of proton deficit followed by a sharp enhancement of proton density. These features are produced by gradients in propagating compressed magnetic field. We compare the data to the results of 3D PIC simulations of plasma collisions, and describe the signatures of magnetized shock formation, including the early electrostatic-dominated stage, and a later magnetic reflection with magnetic overshoots. We point out the importance of the contact discontinuity between the flows, and its dependence on the magnetization of plasma. We explain the geometrical effects on the radiography introduced by density gradients in expanding plasma and by the curvature of the imposed magnetic field. We conclude that our experiments have reproducibly achieved magnetized shocks with Alfvenic Mach number 3 to 9 in laboratory conditions. |
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