In-source decay (ISD) is a rapid fragmentation occurring in the matrix-assisted laser desorption/ionization (MALDI) source before the ion extraction. Despite the increasing interest for peptides de novo sequencing by ISD, the influence of the matrix and of the peptide itself is not yet fully understood. Here we compare matrices with high ISD efficiencies to gain deeper insight in the ISD fragmentation process(es). The major ISD fragments are the c-and z-ions, but other types of fragments are also observed, and their origin is studied here. Two main pathways lead to fragmentation in the source: a radical-induced pathway that leads to c-, z-, w-, and d-ions, and a thermally activated pathway that leads to y-, b-, and a-ions. A detailed analysis of the ISD spectra of selected peptides revealed that (1) the extents of the two in-source pathways are differently favored depending on the matrix used, that (2) the presence of a positive/negative charge on the radical-induced fragments is necessary for their observation in positive/negative mode, respectively, and that (3) [4 -9], especially peptides and proteins. In-source decay (ISD) [10,11] is a fragmentation occurring in the MALDI source, rapidly after the laser shot and before the ion extraction. ISD fragments are therefore detected at the correct m/z ratios in MS mode. On the contrary, fragments formed after the ion extraction are not resolved in MS mode, and can only be revealed by MS/MS in dual stage time-of-flight instruments [12], or by a stepwise lowering of the reflectron voltage in the so-called PSD (post source decay) mode [13,14]. ISD of peptides and proteins mainly leads to c-and z-ions [15,16], and the consensus explanation is that those fragments come from a reduction of the parent ion by hydrogen radicals coming from the matrix [17,18]. Nevertheless, other fragments such as a-, b-, and y-ions have also been reported to form in the MALDI source [4, 7-9, 19, 20]. PSD leads mainly to similar fragments as those formed by low-energy collision-induced dissociation (a-, b-, and y-ions) [21,22].Contrary to CID-like fragments, the radical-induced ISD fragments (c-and z-ions) have the advantage of being theoretically not limited in mass. Indeed, in CID experiments, the internal energy received by the peptide is distributed amongst all its degrees of freedom, i.e., they undergo intramolecular vibrational-energy redistribution (IVR). Therefore, the larger the peptide, the less the energy received per degree of freedom, decreasing the fragmentation efficiency. Like in electron capture dissociation (ECD) [23,24], because the production of c-and z-ions results from a radical-driven process that takes place before the completion of the IVR (non-ergodic process), ISD fragmentation efficiency does not depend on the mass of the peptide and allows to sequence larger peptides as well as intact proteins [5,10].In the present work, we address the mechanisms of in-source formation of the different fragment types. The difficulty in addressing these mechanisms comes from the f...