Knudsen layer formation in laser induced thermal desorption

TL;DR

This study investigates the formation of the Knudsen layer during laser-induced thermal desorption of xenon atoms, revealing how flow dynamics change with coverage and confirming theoretical predictions about Knudsen layer development.

Contribution

It provides experimental evidence of Knudsen layer formation in laser desorption and quantifies the flow velocity and temperature parameters across different coverages.

Findings

Flow follows Maxwell-Boltzmann distribution at low coverage

Stream velocity increases with coverage and saturates at high coverage

Knudsen layer formation completes at Knudsen number less than 0.39

Abstract

Laser induced thermal desorption of Xe atoms into vacuum from a metal surface following the nano-second pulsed laser heating was investigated by the time-of-flight (TOF) measurement. The desorption flow was studied at a wide range of desorption flux by varying the initially prepared Xe coverage {\Theta} (1 ML = 4.5*10^18 atoms/m^2). At {\Theta} = 0.3 ML, the TOF of Xe was well represented by a Maxwell-Boltzmann velocity distribution, which is in good agreement with thermal desorption followed by collision-free flow. At {\Theta} > 0.3 ML, the peak positions of the TOF spectra were shifted towards the smaller values and became constant at large {\Theta}, which were well fitted with a shifted Maxwell-Boltzmann velocity distribution with a temperature T_D and a stream velocity u. With T_D fixed at 165 K, u was found to increase from 80 to 125 m/ s with increasing {\Theta} from 1.2 to 4 ML. At {\Theta} > 4 ML, the value of u become constant at 125 m/ s. The converging feature of u was found to be consistent with analytical predictions and simulated results based on the Knudsen layer formation theory. We found that the Knudsen layer formation in laser desorption is completed at Knudsen number Kn <0.39.