TY - JOUR
T1 - Optimization of the discrete pulse sequence for two-dimensional FT-ICR mass spectrometry using infrared multiphoton dissociation
AU - Van Agthoven, Maria A.
AU - Chiron, Lionel
AU - Coutouly, Marie Aude
AU - Sehgal, Akansha Ashvani
AU - Pelupessy, Philippe
AU - Delsuc, Marc André
AU - Rolando, Christian
N1 - Funding Information:
The authors thank Mr. Fabrice Bray, Dr. Caroline Tokarski, Dr. Alexia Ortiz and Dr. Sophie Dallongeville for helpful conversations. We thank Dr. Andreas Krause from Bruker Daltonics for sharing information on the power amplifier of the AQS system on the 9.4T ApexQE FT-ICR instrument. The FT-ICR mass spectrometer and the Proteomics Platform used for this study are funded by the European community (FEDER) , the Région Nord-Pas de Calais (France) , the IBISA network , the CNRS and the Université Lille 1, Sciences et Technologies , which are gratefully acknowledged. M.v.A. thanks the Région Nord Pas-de-Calais for postdoc funding. This 2D FT-ICR project was funded by the Agence Nationale de la Recherche in 2010 (FT-ICR 2D). Financial support from the TGE CNRS FT-ICR and from the Défi interdisciplinaire CNRS Instrumentation aux limites for conducting the research is also gratefully acknowledged.
PY - 2014/9/15
Y1 - 2014/9/15
N2 - 2D FT-ICR MS, introduced by Pfändler et al. (Chem. Phys. Lett. 138 (1987) 195), allows one to correlate precursor and fragment ions in complex samples without requiring ion isolation. Recent advances in electronics, computer capacities, and gas-free in-cell fragmentation techniques open up new perspectives for 2D FT-ICR MS as an analytical technique. The pulse sequence consists of two encoding pulses separated by an incremental delay, followed by an observe pulse. In our previous 2D FT-ICR MS work we used three pulses of equal duration and amplitude. However, signal intensity was low because it was distributed over a series of intense harmonics. Using a simple theoretical model to analytically express ion fragmentation and 2D FT-ICR MS ion trajectories, we obtained a nearly pure signal when the maximum radius of the ions during the encoding pulses is within the laser beam. By adjusting the experimental parameters of the encoding pulses according to the calculation on the same cyclotron radius, we strongly decrease the intensity of harmonic peaks. We also discuss the effect of increasing the amplitude of the observe pulse, which affects precursor and fragment ion peaks differently in terms of signal-to-noise ratio. The 2D mass spectra obtained with the optimized pulse sequence show a much higher signal-to-noise ratio, even without using denoising algorithms.
AB - 2D FT-ICR MS, introduced by Pfändler et al. (Chem. Phys. Lett. 138 (1987) 195), allows one to correlate precursor and fragment ions in complex samples without requiring ion isolation. Recent advances in electronics, computer capacities, and gas-free in-cell fragmentation techniques open up new perspectives for 2D FT-ICR MS as an analytical technique. The pulse sequence consists of two encoding pulses separated by an incremental delay, followed by an observe pulse. In our previous 2D FT-ICR MS work we used three pulses of equal duration and amplitude. However, signal intensity was low because it was distributed over a series of intense harmonics. Using a simple theoretical model to analytically express ion fragmentation and 2D FT-ICR MS ion trajectories, we obtained a nearly pure signal when the maximum radius of the ions during the encoding pulses is within the laser beam. By adjusting the experimental parameters of the encoding pulses according to the calculation on the same cyclotron radius, we strongly decrease the intensity of harmonic peaks. We also discuss the effect of increasing the amplitude of the observe pulse, which affects precursor and fragment ion peaks differently in terms of signal-to-noise ratio. The 2D mass spectra obtained with the optimized pulse sequence show a much higher signal-to-noise ratio, even without using denoising algorithms.
KW - 2-dimensional
KW - FT-ICR
KW - FTMS
KW - IRMPD
KW - Optimization
KW - Pulse sequence
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U2 - 10.1016/j.ijms.2014.06.019
DO - 10.1016/j.ijms.2014.06.019
M3 - Article
AN - SCOPUS:84904317662
SN - 1387-3806
VL - 370
SP - 114
EP - 124
JO - International Journal of Mass Spectrometry
JF - International Journal of Mass Spectrometry
ER -