On the influence of Alfvén resonance on ion cyclotron resonance heating A. V. Timofeev Methods of Plasma Heating 29 January 2014 Pages: 1 - 13
Influence of the solar wind on the distribution of the electric potential near the Moon’s surface T. M. Burinskaya Space Plasma 29 January 2014 Pages: 14 - 20
Time evolution of the plasma spatial structure during the formation of a current sheet in argon according to holographic interferometry G. V. OstrovskayaA. G. Frank Plasma Dynamics 29 January 2014 Pages: 21 - 33
Specific features of the kinetics of H2-O2-O2(a 1Δ g ) mixtures: I. formation and quenching of electronically and vibrationally excited (A′) molecules in H2-O2-O2(A 1Δ g ) mixtures at a temperature of 300 K A. A. ChukalovskyT. V. RakhimovaO. V. Proshina Low-Temperature Plasma 29 January 2014 Pages: 34 - 51
Specific features of the kinetics of H2-O2-O2(a 1Δ g ) mixtures: II. Quenching of O2(a 1Δ g ) excited in a discharge behind the shock front at temperatures of 500–1020 K A. A. ChukalovskyT. V. RakhimovaO. V. Proshina Low-Temperature Plasma 29 January 2014 Pages: 52 - 64
Mechanism of streamer stopping in a surface dielectric barrier discharge V. R. SolovievV. M. Krivtsov Low-Temperature Plasma 29 January 2014 Pages: 65 - 77
Separation of the heavy and light ion components in a plasma flow propagating in a curvilinear magnetic field V. L. PapernyiN. V. Lebedev Low-Temperature Plasma 29 January 2014 Pages: 78 - 82
Near-magnetic-axis geometry of a closely quasi-isodynamic stellarator M. I. MikhailovJ. NührenbergR. Zille Brief Communications 29 January 2014 Pages: 83 - 87