Electron-temperature control is performed on plasmas passing through a
coarse mesh grid from a discharge region. By increasing a negative po
tential applied to the grid, the electron temperature is continuously
decreased in a very wide range covering almost two orders of magnitude
down to the value nearly equal to the background gas temperature in c
ase of direct current argon or helium gas discharge. The temperature d
ecrease is accompanied by an increase in the electron density. This me
thod of electron-temperature control can also be applied to plasmas pr
oduced by radio-frequency and electron cyclotron resonance discharges.