). A hollow cathode arc as a high intensity beam source for ground state and metastable noble gas atoms in the eV translational energy range. Journal of Physics E: Scientific Instruments, 15(5), 573-579. DOI: 10.1088/0022-3735/15/5/023General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights.• Users may download and print one copy of any publication from the public portal for the purpose of private study or research.• You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal ?
Take down policyIf you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim.Download date: 11. May. 2018 J. Phys. E: Sci. Instrum.? Vol. 15, 1982. Printed in Great Britain such a value that the ion temperature Ti approaches the electron temperature T,. With T, in the order of 3-10eV the ion temperature will vary from 0.2 to a few eV. Fast ground state atoms are produced in collisions between ions and atoms, i.e. charge exchange and elastic collisions. This results in ground state atoms in the desired velocity range. Because the intensity of the resulting beam depends on the product of the neutral and ion density, we expect optimum results for a highly ( Z 50%) ionised plasma. Fast metastable atoms are produced by collisions between electrons and fast ground state atoms (excitation) and between ions and slow metastable atoms with charge exchange. Maximum intensities are expected for high T, and a high neutral density.As these plasma conditions are met in a magnetically stabilised hollow cathode arc (HcA),we have chosen to use this type of discharge.A hollow cathode arc as a high intensity beam source for ground state and metastable noble gas atoms in the eV translational energy range Abstract. The medium density plasma column ( n z close to the exit of the cathode of a hollow cathode arc is highly ionised. with ion and electron temperatures T, ~0 . 5 -1 . 5 eV and T, z 3 eV, respectively. By sampling this plasma with an orifice in the end anode (at a floating potential) a high intensity beam with a broad velocity distribution is obtained for the noble gas a t o m Ne, Ar and Kr. both in the ground state and in metastable states n*. Typical centre-line intensities for argon are I(0) = 2 x lo1* s-l sr-', T= 2 x lo4 K and I(0)n. = 2 x 1014 s-' sr-'. T,. = 3 x lo4 K. These values are in good agreement with model calculations of the process of molecular beam sampling, which are discussed in this paper. The source is of a simple design and easy to operate. The life time of the tungsten (or tantalum) hollow cathode is typically 40 h for argon and krypton. The shortest life time is for...