Anomalies in the Process of Ionization of Analytes in MALDI: Electronic Transfer Vs. Proton Transfer Via Quantum Chemistry

Matrix-Assisted Laser Ionization/Desorption (MALDI) makes possible to ionize any target molecule (with low or high molecular weight and/or with low or high concentration) indirectly, mediated by analyte interaction with with an organic compound that serves as a matrix. The FisicoQuímica Teórica y Ex...

Full description

Bibliographic Details
Main Authors: María J. Álvarez, Luis Miguel Díaz Sánchez, Marianny Yajaira Combariza Montañez, Cristian Blanco Tirado, Aldo Fabrizzio Combariza Montañez
Format: Conference Object
Language:unknown
Published: 2022
Subjects:
Uis
Online Access:https://zenodo.org/record/6481582
https://doi.org/10.5281/zenodo.6481582
Description
Summary:Matrix-Assisted Laser Ionization/Desorption (MALDI) makes possible to ionize any target molecule (with low or high molecular weight and/or with low or high concentration) indirectly, mediated by analyte interaction with with an organic compound that serves as a matrix. The FisicoQuímica Teórica y Experimental (GIFTEX) Research Group of the Universidad Industrial de Santander (UIS) have been working for years on the development of MALDI matrices for the analysis of a broad spectrum of chemical species. Matrixes developed by GIFTEX-RG, such as ????-cyanophenylenevinylene (????-CNFV), are suggested as better analytical medators than commercial matrices, such as DCTB. Therefore, we propose the use of mechano-quantum methods to calculate physical-chemical parameters of the compounds involved in the study (matrixes and analytes) to evaluate CNFV as possible Proton Transfer (PT) matrices. The first step is to obtain the geometries of matrix and analyte structures, followed by geometry optimization, using the quantum chemistry software ORCA, both in neutral and protonic chemical state. Geometry optimizations will be performed using ab initio (RHF/6-311G(2d,2p)) and DFT (B3LYP/6-311G(2d,2p)) theory levels. Later on, the system energy and the most favorable protonation site will be evaluated. Calculations will be performed in gaseous phase, subtracting the energy difference between the neutral optimised structure and the protonate optimised structure. The results will be analyzed to explain the anomalous protonation of analytes using electron transfer matrices.