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Fourier transform ion cyclotron resonance mass spectrometer with coaxial multi‐electrode cell (‘O‐trap’): first experimental demonstration
Author(s) -
Misharin A. S.,
Zubarev R. A.,
Doroshenko V. M.
Publication year - 2010
Publication title -
rapid communications in mass spectrometry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.528
H-Index - 136
eISSN - 1097-0231
pISSN - 0951-4198
DOI - 10.1002/rcm.4593
Subject(s) - fourier transform ion cyclotron resonance , ion cyclotron resonance , chemistry , ion trap , coaxial , cyclotron , atomic physics , quadrupole ion trap , mass spectrometry , ion , analytical chemistry (journal) , excitation , nuclear magnetic resonance , physics , electrical engineering , organic chemistry , quantum mechanics , engineering , chromatography
Abstract The conceptual design of the O‐trap Fourier transform ion cyclotron resonance (FT‐ICR) cell addresses the speed of analysis issue in FT‐ICR mass spectrometry. The concept of the O‐trap includes separating the functions of ion excitation and detection between two different FT‐ICR cell compartments. The detection compartment of the O‐trap implements additional internal coaxial electrodes around which ions with excited cyclotron motion revolve. The expected benefits are higher resolving power and the lesser effect of the space charge. In this work we present the first experimental demonstration of the O‐trap cell and its features, including the high ion transfer efficiency between two distinct compartments of an ICR cell after excitation of the coherent cyclotron motion. We demonstrate that utilization of the multiple‐electrode detection in the O‐trap provides mass resolving power enhancement (achieved over a certain time) equal to the order of the frequency multiplication. In an O‐trap installed in a 5 T desk‐top cryogen‐free superconducting magnet, the resolving power of R = 80 000 was achieved for bradykinin [M + 2H] 2+ ( m/z 531; equivalent to 100 000 when recalculated for m/z 400) in 0.2 s analysis time (transient length), and R = 300 000 at m/z 531 for a 1 s transient. In both cases, detection on the third multiple of the cyclotron frequency was implemented. In terms of the acquisition speed at fixed resolving power, such performance is equivalent to conventional FT‐ICR detection using a 15 T magnet. Copyright © 2010 John Wiley & Sons, Ltd.