The emission of Rydberg states of alkali atoms by thermal desorption a
t high-temperature surfaces can be studied by the field reversal (FR)
rapid kinetics method. This method is based on molecular beam steady-s
tate conditions with periodic reversals of the electric field outside
the hot surface to modulate the desorbing flux. Such a modulation is p
ossible if the ion desorption channel is larger than or of the same si
ze as the neutral desorption channel. The desorption of K was studied
on carbon-covered Ir and partly oxidized Re surfaces with rise and fal
l times of the field of less than 10 ns, and with field strengths as l
ow as 5 V cm(-1). The existence of Rydberg states K was verified from
the very large, 300-ns-broad first ion peak after field reversal to a
ccelerating field. The size of this peak was sensitive to the conditio
ns during the retarding phase, which shows that it was caused by ioniz
ation of K emitted during the retarding phase. The formation of Rydbe
rg species was also verified by extraction of ions even during the ret
arding phase, with the temporal dependence following the accumulation
of K-atoms on the surface. The ion extraction in this case was due to
field ionization of desorbing K at very low field strengths. The ion
formation was not due to field penetration, since the typical FR time
dependence during the retarding phase was retained. The positive curre
nt extracted at low emitter voltages under constant field conditions a
lso supports this view. Electron current emission studies in fields wi
th reversed polarity neither showed any field penetration. The thermal
excitation barrier was found to be 4.31 +/- 0.24 eV, which agrees wit
h the excitation energy for Rydberg states K. (C) 1998 Elsevier Scien
ce B.V. All rights reserved.