Vlasov simulations of plasma-wall interactions in a magnetized and weakly collisional plasma

A Vlasov code is used to model the transition region between an equilibrium plasma and an absorbing wall in the presence of a tilted magnetic field, for the case of a weakly collisional plasma (λmfp≫ρi, where λmfp is the ion-neutral mean-free path and ρi is the ion Larmor radius). The phase space structure of the plasma-wall transition is analyzed in detail and theoretical estimates of the magnetic presheath width are tested numerically. It is shown that the distribution near the wall is far from Maxwellian, so that temperature measurements should be interpreted with care. Particular attention is devoted to the angular distribution of ions impinging on the wall, which is an important parameter to determine the level of wall erosion and sputtering.

[1]  Plasma Flow in the Sheath and the Presheath of a Scrape-Off Layer , 1986 .

[2]  Douglass E. Post,et al.  Physics of Plasma-Wall Interactions in Controlled Fusion , 1986, Springer US.

[3]  D. Tskhakaya,et al.  On the theory of plasma-wall transition layers , 2004 .

[4]  J. Chutia,et al.  Experimental observation of sheath and magnetic presheath over an oblique metallic plate in the presence of a magnetic field , 2002 .

[5]  E. Ahedo Structure of the plasma-wall interaction in an oblique magnetic field , 1997 .

[6]  N. Hershkowitz,et al.  Experimental studies of the Bohm criterion in a two-ion-species plasma using laser-induced fluorescence. , 2003, Physical review letters.

[7]  David Tskhakaya,et al.  The Magnetised Plasma‐Wall Transition: Theory and PIC Simulation , 2004 .

[8]  G. Bonhomme,et al.  Low-frequency instabilities in a laboratory magnetized plasma column , 2004 .

[9]  R. K. Wakerling,et al.  The characteristics of electrical discharges in magnetic fields , 1949 .

[10]  G. Manfredi,et al.  Kinetic simulations of ion temperature measurements from retarding field analyzers , 2002 .

[11]  K. Riemann,et al.  Kinetic analysis of the plasma boundary layer in an oblique magnetic field , 1999 .

[12]  R. Chodura,et al.  Plasma–wall transition in an oblique magnetic field , 1982 .

[13]  G. Knorr,et al.  The integration of the vlasov equation in configuration space , 1976 .

[14]  Chung,et al.  Kinetic theory of ion collection by probing objects in flowing strongly magnetized plasmas. , 1988, Physical review. A, General physics.

[15]  P. Stangeby The Plasma Boundary of Magnetic Fusion Devices , 2000 .

[16]  D. Tskhakaya,et al.  Kinetic (PIC) simulations of the magnetized plasma–wall transition , 2005 .

[17]  K. Riemann Theory of the collisional presheath in an oblique magnetic field , 1994 .

[18]  J. Gunn The influence of magnetization strength on the sheath: Implications for flush-mounted probes , 1997 .

[19]  D. Sharma Kinetic Lagrange simulation of a source-driven magnetized oblique presheath , 2005 .

[20]  D. Tskhakaya,et al.  Effects of energetic electrons on magnetized electrostatic plasma sheaths , 2002 .

[21]  Giovanni Manfredi,et al.  Vlasov simulations of plasma-wall interactions in a weakly collisional plasma , 2004, Comput. Phys. Commun..

[22]  E. Fijalkow,et al.  A numerical solution to the Vlasov equation , 1999 .