Search Results - "FINN, J. M"

An optimal robust equidistribution method for two-dimensional grid adaptation based on Monge–Kantorovich optimization by Delzanno, G.L., Chacón, L., Finn, J.M., Chung, Y., Lapenta, G.

“…A new cell-area equidistribution method for two-dimensional grid adaptation, based on Monge–Kantorovich optimization (or Monge–Kantorovich optimal transport),…”
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Rossby Wave Instability of Thin Accretion Disks. II. Detailed Linear Theory by Li, H, Finn, J. M, Lovelace, R. V. E, Colgate, S. A

“…In an earlier work we identified a global, nonaxisymmetric instability associated with the presence of an extreme in the radial profile of the key function…”
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Quasi-separatrix layers and three-dimensional reconnection diagnostics for line-tied tearing modes by Richardson, A.S., Finn, J.M.

“…► We study a model of line-tied MHD modes, with no nulls or closed field lines. ► We analyze quasi-separatrix layers, the squashing factor, and two scalar…”
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Noise and error analysis and optimization in particle-based kinetic plasma simulations by Evstatiev, E.G., Finn, J.M., Shadwick, B.A., Hengartner, N.

“…•Numerical noise is studied in a finite particle number system, by kernel density estimation.•Ornstein-Uhlenbeck bridge describes the electric field…”
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An Implicit, Nonlinear Reduced Resistive MHD Solver by Chacón, L., Knoll, D.A., Finn, J.M.

“…Implicit time differencing of the resistive magnetohydrodynamic (MHD) equations can step over the limiting time scales—such as Alfvén time scales—to resolve…”
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Meshfree Methods for Plasma Kinetic Theory by Finn, J. M., Shadwick, B.

“…We revisit a meshfree particle method for kinetic theory. We first treat a 1D electrostatic plasma with immobile ions. We find the electron density by kernel…”
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What It Means to Be a Global University during a Pandemic by Knoll-Finn, M. J

“…Leading through a pandemic shifted how enrollment management offices leverage their global networks. At New York University (NYU), leaders identified: what it…”
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Magnetic Helix Formation Driven by Keplerian Disk Rotation in an External Plasma Pressure: The Initial Expansion Stage by Li, H, Lovelace, R. V. E, Finn, J. M, Colgate, S. A

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Robust, multidimensional mesh-motion based on Monge–Kantorovich equidistribution by Chacón, L., Delzanno, G.L., Finn, J.M.

“…Mesh-motion (r-refinement) grid adaptivity schemes are attractive due to their potential to minimize the numerical error for a prescribed number of degrees of…”
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The numerical simulation of stretch flange forming by Worswick, M.J., Finn, M.J.

“…Simulations of stretch flange forming operations are undertaken using explicit dynamic finite element calculations utilizing various quadratic and…”
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Modeling the Large-Scale Structures of Astrophysical Jets in the Magnetically Dominated Limit by Li, Hui, Lapenta, Giovanni, Finn, John M, Li, Shengtai, Colgate, Stirling A

“…We suggest a new approach that could be used for modeling both the large-scale behavior of astrophysical jets and the magnetically dominated explosions in…”
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A Magnetic α-ω Dynamo in AGN Disks. II. Magnetic Field Generation, Theories, and Simulations by Pariev, Vladimir I, Colgate, Stirling A, Finn, J. M

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Use of a coupled explicit—implicit solver for calculating spring-back in automotive body panels by Finn, M.J., Galbraith, P.C., Wu, L., Hallquist, J.O., Lum, L., Lin, T.-L.

“…LS-DYNA3D, an explicit code, and LS-NIKE3D, an implicit code, have been coupled to facilitate the finite element (FE) modelling of sheet metal forming. The…”
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Noise and error analysis and optimization in particle-based kinetic plasma simulations by Evstatiev, E. G, Finn, J. M, Shadwick, B. A, Hengartner, N

“…We analyze the noise in macro-particle methods used in plasma physics and fluid dynamics, leading to approaches for minimizing the total error, focusing on…”
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Erratum: Comparison of Polarization Observables in Electron Scattering from the Proton and Deuteron [Phys. Rev. Lett. 80, 452 (1998)] by Milbrath, B. D., McIntyre, J. I., Armstrong, C. S., Barkhuff, D. H., Bertozzi, W., Chen, J. P., Dale, D., Dodson, G., Dow, K. A., Epstein, M. B., Farkhondeh, M., Finn, J. M., Gilad, S., Jones, M. K., Joo, K., Kelly, J. J., Kowalski, S., Lourie, R. W., Madey, R., Margaziotis, D. J., Markowitz, P., Mertz, C., Mitchell, J., Perdrisat, C. F., Punjabi, V., Qin, L., Rutt, P. M., Sarty, A. J., Tieger, D., Tschalær, C., Turchinetz, W., Ulmer, P. E., Van Verst, S. P., Warren, G. A., Weinstein, L. B., Woo, R. J.

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Hall MHD effects on the 2D Kelvin–Helmholtz/tearing instability by Chacón, L., Knoll, D.A., Finn, J.M.

“…The Kelvin–Helmholtz (KHI)/tearing (TMI) instability is studied with a 2D incompressible Hall MHD model. In the equilibrium configuration of interest, the…”
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{sup 2}H(e,e'p)n Reaction at High Recoil Momenta by P. E. Ulmer, K. A. Aniol, H. Arenhoevel, J.-P. Chen, E. Chudakov, D. Crovelli, J. M. Finn, K. G. Fissum, O. Gayou, J. Gomez, J.-O. Hansen, C. W. de Jager, S. Jeschonnek, M. K. Jones, M. Kuss, J. J. LeRose, M. Liang, R. A. Lindgren, S. Malov, D. Meekins, R. Michaels, J. Mitchell, C. F. Perdrisat, V. Punjabi, R. Roche, F. Sabatie, A. Saha, R. Suleiman, L. Todor, B. B. Wojtsekhowski

“…The 2H(e,ep)n cross section was measured in Hall A of the Thomas Jefferson National Accelerator Facility near the top of the quasielastic peak (xBj = 0.964) at…”
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Precision measurement of the weak charge of the proton by Androić, D, Armstrong, D S, Asaturyan, A, Averett, T, Balewski, J, Bartlett, K, Beaufait, J, Beminiwattha, R S, Benesch, J, Benmokhtar, F, Birchall, J, Carlini, R D, Cornejo, J C, Dusa, S Covrig, Dalton, M M, Davis, C A, Deconinck, W, Diefenbach, J, Dowd, J F, Dunne, J A, Dutta, D, Duvall, W S, Elaasar, M, Falk, W R, Finn, J M, est, T, Gal, C, Gaskell, D, Gericke, M T W, Grames, J, Gray, V M, Grimm, K, Guo, F, Hoskins, J R, Jones, D, Jones, M, Jones, R, Kargiantoulakis, M, King, P M, Korkmaz, E, Kowalski, S, Leacock, J, Leckey, J, Lee, A R, Lee, J H, Lee, L, MacEwan, S, Mack, D, Magee, J A, Mahurin, R, Mammei, J, Martin, J W, McHugh, M J, Meekins, D, Mei, J, Mesick, K E, Michaels, R, Micherdzinska, A, Mkrtchyan, A, Mkrtchyan, H, Morgan, N, Narayan, A, Ndukum, L Z, Nelyubin, V, Nuhait, H, Nuruzzaman, van Oers, W T H, Opper, A K, Page, S A, Pan, J, Paschke, K D, Phillips, S K, Pitt, M L, Poelker, M, Rajotte, J F, Ramsay, W D, Roche, J, Sawatzky, B, Seva, T, Shabestari, M H, Silwal, R, Simicevic, N, Smith, G R, Solvignon, P, Spayde, D T, Subedi, A, Subedi, R, Suleiman, R, Tadevosyan, V, Tobias, W A, Tvaskis, V, Waidyawansa, B, Wang, P, Wells, S P, Wood, S A, Yang, S, Young, R D, Zang, P, Zhamkochyan, S

“…Large experimental programmes in the fields of nuclear and particle physics search for evidence of physics beyond that explained by current theories. The…”
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Noise-stabilized random attractor by Finn, J M, Tracy, E R, Cooke, W E, Richardson, A S

“…A two-dimensional flow model is introduced with deterministic behavior consisting of bursts that become successively larger, with longer interburst time…”
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Quasielastic 3He(e, e'p)2H reaction at Q2 = 1.5 GeV2 for recoil momenta up to 1 GeV/c by RVACHEV, M. M, BENMOKHTAR, F, CHEN, J.-P, CHUDAKOV, E, CISBANI, E, COCHRAN, A, CORNEJO, J, DIETERICH, S, DJAWOTHO, P, DURAN, W, EPSTEIN, M. B, FINN, J. M, PENEL-NOTTARIS, E, FISSUM, K. G, FRAHI-AMROUN, A, FRULLANI, S, FURGET, C, GARIBALDI, F, GAYOU, O, GILAD, S, GILMAN, R, GLASHAUSSER, C, HANSEN, J.-O, ANIOL, K. A, HIGINBOTHAM, D. W, HOTTA, A, HU, B, IODICE, M, IOMNI, R, DE JAGER, C. W, JIANG, X, JONES, M. K, KELLY, J. J, KOX, S, BERTOZZI, W, KUSS, M, LAGET, J. M, DE LEO, R, LEROSE, J. J, LIATARD, E, LINDGREN, R, LIYANAGE, N, LOURIE, R. W, MALOV, S, MARGAZIOTIS, D. J, BOEGLIN, W. U, MARKOWITZ, P, MERCHEZ, F, MICHAELS, R, MITCHELL, J, MOUGEY, J, PERDRISAT, C. F, PUNJABI, V. A, QUEMENER, G, RANSOME, R. D, REAL, J.-S, BUTARU, F, CALARCO, J. R, CHAI, Z, CHANG, C. C

“…We have studied the quasielastic 3He(e,e'p)2H reaction in perpendicular coplanar kinematics, with the energy and the momentum transferred by the electron fixed…”
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