Zwitterionic states in gas-phase polypeptide ions revealed by 157-nm ultra-violet photodissociation.

A new method of detecting the presence of deprotonation and determining its position in gas-phase polypeptide cations is described. The method involves 157-nm ultra-violet photodissociation (UVPD) and is based on monitoring the losses of CO2 (44 Da) from electronically excited deprotonated carboxylic groups relative to competing COOH losses (45 Da) from neutral carboxylic groups. Loss of CO2 is a strong indication of the presence of a zwitterionic [(+)...(-)...(+)] salt bridge in the gas-phase polypeptide cation. This method provides a tool for studying, for example, the nature of binding within polypeptide clusters. Collision-activated dissociation (CAD) of decarboxylated cations localizes the position of deprotonation. Fragment abundances can be used for the semiquantitative assessment of the branching ratio of deprotonation among different acidic sites, however, the mechanism of the fragment formation should be taken into account. Cations of Trp-cage proteins exist preferentially as zwitterions, with the deprotonation position divided between the Asp9 residue and the C terminus in the ratio 3:2. The majority of dications of the same molecule are not zwitterions. Furthermore, 157-nm UVPD produces abundant radical cations M*+ from protonated molecules through the loss of a hydrogen atom. This method of producing M*+ ions is general and can be applied to any gas-phase peptide cation. The abundance of the molecular radical cations M*+ produced is sufficient for further tandem mass spectrometry (MS/MS), which, in the cases studied, yielded side-chain loss of a basic amino acid as the most abundant fragmentation channel together with some backbone cleavages.

Dissociation of peptide ions by fast atom bombardment in a quadrupole ion trap.

A new technique for fragmentation of cations and anions of peptides stored in ion traps including radiofrequency devices is described. The technique involves irradiation of peptide ions by a beam of particles generated by a fast atom bombardment (FAB) gun. This irradiation leads to fragmentation of N--C(alpha) backbone bonds (c- and z-fragments) and S--S bonds for cations and C(alpha)-C backbone bonds (a- and x-fragments) for anions of peptides. The fragmentation patterns observed are hypothesized to be due to the interaction of peptide ions with metastable, electronically excited species generated by the FAB gun. Interaction of a metastable atom A* with a peptide n-cation M(n+) leads to the electron transfer from the metastable atom to the polycation through the formation of an ion-pair collision complex A(+.) . . . M((n-1)+.) and subsequent fragmentation of the peptide cation. Thus, for polycations, this metastable-induced dissociation of ions (MIDI) is similar to the phenomenon of electron capture dissociation (ECD). Interaction of A* with an anion leads to the deexcitation of the metastable species and detachment of an electron from the anion. This in turn leads to backbone fragmentation similar to that in electron detachment dissociation (EDD). The MIDI technique is robust and efficient, and it is applicable to peptides in as low charge states as 2+ or 2-.

C alpha-C backbone fragmentation dominates in electron detachment dissociation of gas-phase polypeptide polyanions.

Fragmentation of peptide polyanions by electron detachment dissociation (EDD) has been induced by electron irradiation of deprotonated polypeptides [M-nH](n-) with >10 eV electrons. EDD has been found to lead preferentially to a* and x fragment ions (C(alpha)-C backbone cleavage) arising from the dissociation of oxidized radical anions [M-nH]((n-1)-*. We demonstrate that C(alpha)-C cleavages, which are otherwise rarely observed in tandem mass spectrometry, can account for most of the backbone fragmentation, with even-electron x fragments dominating over radical a* ions. Ab initio calculations at the B3 LYP level of theory with the 6-311+G(2 p,2 d)//6-31+G(d,p) basis set suggested a unidirectional mechanism for EDD (cleavage always N-terminal to the radical site), with a*, x formation being favored over a, x* fragmentation by 74.2 kJ mol(-1). Thus, backbone C(alpha)-C bonds N-terminal to proline residues should be immune to EDD, in agreement with the observations. EDD may find application in mass spectrometry for such tasks as peptide sequencing and localization of labile post-translational modifications, for example, those introduced by sulfation and phosphorylation. EDD can now be performed not only in Fourier transform mass spectrometry, but also in far more widely used quadrupole (Paul) ion traps.

Electron capture dissociation of polypeptides in a three-dimensional quadrupole ion trap: Implementation and first results.

The adverse influence of the radio frequency (RF) voltage on electrons has been the main obstacle for the implementation of electron capture dissociation (ECD) in three-dimensional quadrupole ion traps (3D QITs). Here we demonstrate that the use of axial magnetic field, together with the injection of low-energy (<5 eV) electrons, in the beginning of the positive RF semi-period achieves trapping of electrons for a period of time comparable with the semi-period duration. Importantly, the energy of the electrons remains low during most of the trapping period. With this technique, which we call "magnetized electrons, in-phase injection" (MEPhI), ECD and other ion-electron reactions have become possible in a 3D QIT. Initial ECD results, including single-scan data, were obtained with dications of Substance P. The observed secondary fragmentation of ECD fragments indicates that the trapped electrons are still somewhat hotter than desired.