Sh. Guan et Ag. Marshall, EQUILIBRIUM SPACE-CHARGE DISTRIBUTION IN A QUADRUPOLE ION-TRAP, Journal of the American Society for Mass Spectrometry, 5(2), 1994, pp. 64-71
A simple model provides a basis for evaluating the ion spatial distrib
ution in a quadrupole (Paul) ion trap and its effect on the total pote
ntial (trap potential plus space charge) acting on ions in the trap. B
y combining the pseudopotential approximation introduced by Dehmelt 25
years ago with the assumption of thermal equilibrium (leading to a Bo
ltzmann ion energy distribution), the resulting ion spatial distributi
on (for ions of a single mass-to-charge ratio) depends only on total n
umber of ions, trap pseudopotential, and temperature. (The equilibrium
assumption is justified by the high helium bath gas pressure at which
analytical quadrupole ion traps are typically operated.) The electric
potential generated by the ion space charge may be generated from Poi
sson's equation subject to a Boltzmann ion energy distribution. Howeve
r, because the ion distribution depends in tum on the total potential,
solving for the potential and the ion distribution is no longer a sim
ple boundary condition differential equation problem; an iterative pro
cedure is required to obtain a self-consistent result. For the particu
larly convenient operating condition, a(z) = q(z)2/4 [in which a(z) =
-8qU/mrho0(2) OMEGA2, and q(z) = -4qV/mrho0(2) OMEGA2, where U and V a
re direct current and radiofrequency (frequency, OMEGA) voltages appli
ed to the trap, m/q is ion mass-to-charge ratio, and rho0 is the radiu
s of the ring electrode at the z = 0 midplane], both the pseudopotenti
al and the ion distribution become spherically symmetric. The resultin
g one-dimensional problem may be solved by a simple optimization proce
dure. The present model accounts qualitatively for the dependence of t
otal potential and ion distribution on number of ions (higher ion dens
ity or lower temperature flattens the total potential and widens the s
patial distribution of ions) and pseudopotential (higher pseudopotenti
al increases ion density near the center of the trap without widening
the ion spatial distribution).