Open trapped ion cell geometries for Fourier transform ion cyclotron resonance mass spectrometry

Fourier transform ion cyclotron resonance mass spectrometry is evaluated in trapped ion cells which substitute open rectangular trapping electrodes for trapping plates positioned perpendicular to the magnetic field. Compared with closed cells, the open cell geometry offers improved access to the cell interior with obvious benefits for external ion injection. The well depth along the z-axis centerline of the open cell is about 37% of the applied potential for cubic geometry but increases to 81% for an elongated cell with aspect ratio two. Isopotential field maps are created to compare axial and radial components of trapping and excitation fields for open and closed orthorhombic cells. Radial trapping electric fields are somewhat larger in the center of the open cells but axial excitation fields are a factor of two smaller compared with the closed cell. An open elongated cell with an aspect ratio of two is constructed and compared with a closed cell of similar aspect ratio. Experimentally, a −57 Hz V−1 shift in cyclotron frequency owing to the radial trapping field is obtained for the open cell compared with a −32 Hz V−1 shift for the closed cell. However, axial ejection is significantly reduced in the open cell compared with the closed cell. Suggestions are given for generalizing the open cell to a mutisegmented electrode assembly in which excitation, detection and trapping are performed interchangeably with the same electrodes. For example, capacitive coupling of the excitation potential to the trap electrodes is suggested as a simple means of eliminating axial ejection during excitation.

[1]  R. Dunbar,et al.  Magnetron motion of ions in the cubical ICR cell , 1984 .

[2]  J. Degrassie,et al.  Properties of nonneutral plasma , 1975 .

[3]  Melvin B. Comisarow,et al.  Cubic trapped-ion cell for ion cyclotron resonance , 1981 .

[4]  F. McLafferty,et al.  Developments in analytical fourier-transform mass spectrometry , 1985 .

[5]  F. MacKintosh,et al.  Cylindrical Penning traps with orthogonalized anharmonicity compensation , 1984 .

[6]  D. Russell,et al.  Axial magnetic inhomogeneities and low energy ion injection in Fourier-transform ion cyclotron resonance spectrometry , 1989 .

[7]  K. Wanczek,et al.  Coupling of axial and radial motions in ICR cells during excitation , 1986 .

[8]  R. L. Hunter,et al.  An elongated trapped-ion cell for ion cyclotron resonance mass spectrometry with a superconducting magnet , 1983 .

[9]  M. Gross,et al.  Relation of signal sensitivity and ion z-motion in cubic cells. Theory and implication for ion kinetic studies , 1986 .

[10]  A. Marshall,et al.  A "screened" electrostatic ion trap for enhanced mass resolution, mass accuracy, reproducibility, and upper mass limit in Fourier transform ion cyclotron resonance mass spectrometry. , 1989, Analytical chemistry.

[11]  P. Schwinberg,et al.  Preliminary Proton/Electron Mass Ratio using a Compensated Quadring Penning Trap , 1981 .

[12]  C. Chakrabarti,et al.  Effect of pH and uranium concentration on interaction of uranium(VI) and uranium(IV) with organic ligands in aqueous solutions , 1980 .

[13]  K. Wanczek,et al.  Ejection of low-mass charged particles in high magnetic field ICR spectrometers , 1987 .

[14]  P. Caravatti,et al.  The ‘infinity cell’: A new trapped‐ion cell with radiofrequency covered trapping electrodes for fourier transform ion cyclotron resonance mass spectrometry , 1991 .

[15]  A. Marshall,et al.  Fourier Transform Ion Cyclotron Resonance Spectroscopy , 1974 .

[16]  M. Gross,et al.  Parametric mode operation of a hyperbolic Penning trap for Fourier transform mass spectrometry. , 1987, Analytical chemistry.

[17]  T. E. Sharp,et al.  Trapped-ion motion in ion cyclotron resonance spectroscopy , 1972 .

[18]  P. Faragó,et al.  On the production of polarized electron beams by spin exchange collisions , 1965 .

[19]  L. Haarsma,et al.  Open-endcap Penning traps for high precision experiments , 1989 .

[20]  A. Marshall,et al.  Elimination of z-ejection in Fourier transform ion cyclotron resonance mass spectrometry by radio frequency electric field shimming. , 1990, Analytical chemistry.

[21]  J. Hipple,et al.  THE MEASUREMENT OF e/M BY CYCLOTRON RESONANCE , 1951 .

[22]  Robert L. White,et al.  Exact mass measurement by Fourier transform mass spectrometry , 1980 .

[23]  M. Gross,et al.  Mass-dependent z-excitation of ions in cubic traps used in FTMS , 1986 .

[24]  D. Laude,et al.  Ion ejection from fourier transform mass spectrometry trapped ion cells due to non-adiabatic changes in trapping potentials , 1990 .

[25]  D. Russell,et al.  Field-corrected ion cell for ion cyclotron resonance , 1990 .

[26]  J. Degrassie,et al.  Wave-induced transport in the pure electron plasma , 1977 .

[27]  J. Degrassie Equilibrium, waves and transport in the pure electron plasma , 1977 .