The Self-consistent radial electric field at various powers and radio frequencies for hydrogen and helium background gases.

The Self-consistent radial electric field at various powers and radio frequencies for hydrogen and helium background gases.</p

Axial kinetic energy (eV) verses trap radius (m) graphs for hydrogen background gas having density 5×10^-14m^-3 at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF are shown in legend of Fig 4(A)–4(F) for simulation time of 100 μs and powered to C₈ cylinder of realistic trap.

Axial kinetic energy (eV) verses trap radius (m) graphs for hydrogen background gas having density 5×10-14m-3 at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF are shown in legend of Fig 4(A)–4(F) for simulation time of 100 μs and powered to C8 cylinder of realistic trap.</p

Axial kinetic energy (eV) verses trap radius (m) graphs for helium background gas having density 5×10^-14m^-3 at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF are shown in legend of Fig 5(A)–5(F) for simulation time of 100 μs and powered to C₈ cylinder of realistic trap.

Axial kinetic energy (eV) verses trap radius (m) graphs for helium background gas having density 5×10-14m-3 at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF are shown in legend of Fig 5(A)–5(F) for simulation time of 100 μs and powered to C8 cylinder of realistic trap.</p

Simulation input parameters for the confinement of electron plasma.

Simulation input parameters for the confinement of electron plasma.</p

Radial electric field along trap radius at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF shown in legend for hydrogen background gas for simulation time of 100 μs having background gas density 5×10⁻¹⁴ m^-3 and powered to C₈ cylinder in realistic trap.

Radial electric field along trap radius at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF shown in legend for hydrogen background gas for simulation time of 100 μs having background gas density 5×10−14 m-3 and powered to C8 cylinder in realistic trap.</p

Fig 2 -

Axial and radial temperatures verses simulation time at background gases Hydrogen (a, b) and Helium (c, d). The simulation performed at applied constant frequency of 1 GHz resonate with magnetic field 0.035706 tesla of different amplitudes for the cases indicated in the legend applied to C8 cylinder of ELTRAP.</p

Radial electric field along trap radius at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF shown in legend for hydrogen background gas for simulation time of 100 μs having background gas density 5×10⁻¹⁴ m^-3 and powered to C₈ cylinder in realistic trap.

Radial electric field along trap radius at constant RF of 1 GHz for these varying amplitudes as well as for constant amplitude of 3.8 V for these varying RF shown in legend for hydrogen background gas for simulation time of 100 μs having background gas density 5×10−14 m-3 and powered to C8 cylinder in realistic trap.</p

Fig 3 -

Axial and radial temperatures verses simulation time at background gases Hydrogen (a, b) and Helium (c, d). The simulation performed at constant amplitude of 3.8 V for different radio frequencies indicated in legend matched with corresponding magnetic fields are applied to C8 cylinder of ELTRAP.</p

Schematic diagram of ELTRAP for confinement of electron plasma.

Schematic diagram of ELTRAP for confinement of electron plasma.</p