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Infrared multiple photon dissociation (IRMPD) spectroscopy shows the [GPGG + H – H2O]+ ion to have an imidazolone structure. Collision-induced dissociation of this [b4]+ ion results in the loss of HN CH2 from the first residue; the IRMPD spectrum of this MS3 product ion is very similar to that of the [b4]+ ion itself, strongly indicating that the [b4 – HN CH2]+ ion also has an imidazolone structure. Losses of CO and glycine are the dominant dissociation pathways for the [b4 – HN CH2]+ ion. The latter loss requires tautomerism of the keto-form of the imidazolone ring to become the lower-energy enol-form, prior to dissociation. Isotopic labelling showed that loss of CO occurs from the ring of the keto-form. Density functional theory calculations were performed at both the B3LYP/6–311++G (d,p) and M06–2X/6–311++G (d,p) levels and the results are in good agreement.

Synthesis and spectra of isocytosino-8-trifluoromethylquinolone (1), as well as the gas phase InfraRed Multiple Photon Dissociation (IRMPD) spectra in the fingerprint region of the corresponding deprotonated anion (3), its d3 analogue, the monodeprotonated homodimer (2), and its d7 analogue are reported here. The anions represent nucleobase analogues having the hydrogen bonding pattern ADAAD (where A stands for acceptor and D stands for donor), in which the site of negative charge is unambiguous (as opposed to guanine, which has more than one acidic nitrogen). The match between experimental vibrational spectra and calculation is good, except for the out-of-plane HNH bends of the undeuterated and deuterated monomer anions between 400 and 600 cm−1. The anionic homodimers form in a parallel orientation.

The role of specific amino acid side-chains in the fragmentation chemistry of gaseous protonated peptides resulting from collisional activation remains incompletely understood. For small peptides containing asparagine and glutamine, a dominant fragmentation channel induced by collisional activations is, in addition to deamidation, the loss of neutral water. Identifying the product ion structures from H2O-loss from four protonated dipeptides containing Asn or Gln using infrared ion spectroscopy, mechanistic details of the dissociation reactions are revealed. Several sequential dissociation reactions have also been investigated and provide additional insights into the fragmentation chemistry. While water loss can in principle occur from the C-terminus, the side chain or the amide bond carbonyl oxygen, in most cases the C-terminus was found to detach H2O, leading to a b2-sequence ion with an oxazolone structure for AlaGln, and bifurcating mechanisms leading to both oxazolone and diketopiperazine species for AlaAsn and AsnAla. In contrast, GlnAla expels water from the amide side chain leading to an imino-substituted prolinyl structure.

Complexes of divalent metal ions (Cu2+ and Ni2+) with histidine tripeptide complexes (HAA, AHA and AAH) are interesting gas-phase models for some of the most widely observed patterns of metal ion binding to peptides and proteins. Gas-phase structures were characterized using infrared multiple photon dissociation (IRMPD) spectroscopy in ion-trapping mass spectrometers, along with density functional theory (DFT) computations. Ground states are square-planar with two deprotonated amide nitrogens bound to the metal ion via a double iminol rearrangement (IM binding mode), but contrary to expectations based on solution behavior, the histidine imidazole group is not bound to the metal, but instead is hydrogen bonded remote from the metal ion. The alternative “charge-solvated” (CS) binding mode (amide carbonyl oxygens binding the metal ion) lies higher in energy, but in many cases was observed to be present as conformationally unrelaxed ions with an abundance (relative to the IM conformation) that was dependent on instrument configuration and source and trap conditions. Taking advantage of the ability to form and trap both IM and CS conformations for a few of the complexes, the infrared spectroscopy of both conformations was explored in the fingerprint (1000–1800 cm−1) and hydrogen-stretching (3200–3800 cm−1) regions. For the fingerprint region, agreement is very good between the observed IRMPD spectra and the spectra predicted by DFT calculations at the B3LYP/6–311 + +g(d,p) level. Agreement in the H-stretching region is not perfect, but the characteristic IM and CS spectral patterns are evident.

Infrared multiple photon dissociation spectroscopy was performed on protonated and cationized canavanine (Cav), a non-protein amino acid oxy-analog of arginine. Infrared spectra in the XH stretching region (3000–4000 cm−1) were obtained at the Centre Laser Infrarouge d’Orsay (CLIO) facility. Comparison of the experimental infrared spectra with scaled harmonic frequencies at the B3LYP/6-31+G(d,p) level of theory indicates that canavanine is in a canonical neutral form in CavH+, CavLi+, and CavNa+; therefore, these cations are charge-solvated structures. The infrared spectrum of CavK+ is consistent with a mixture of Cav in canonical and zwitterionic forms leading to both charge-solvated and salt-bridged cationic structures. The Cav moiety in CavCs+ is shown to be zwitterionic, forming a salt-bridged structure for the cation. Infrared spectra in the fingerprint region (1000–2000 cm−1) obtained at the FELIX Laboratory in Nijmegen, Netherlands support these assignments. These results show that a single oxygen atom substitution in the side chain reduces the stability of the zwitterion compared to that of the protein amino acid arginine (Arg), which has been shown previously to adopt a zwitterionic structure in ArgNa+ and ArgK+. This difference can be explained in part due to the decreased basicity of Cav (PA = 1001 kJ/mol) as compared to arginine (PA = 1051 kJ/mol), but not entirely, as lysine, which has nearly the same proton affinity as Cav, (∼993 kJ/mol) forms only canonical structures with Na+, K +, and Cs+. A major difference between the zwitterionic forms of ArgM+ and CavM+ is that the protonation site is on the side chain for Arg and on the N-terminus for Cav. This results in systematically weaker salt bridges in the Cav zwitterions. In addition, the presence of another hydrogen-bonding acceptor atom in the side chain contributes to the stability of the canonical structures for the smaller alkali cations.

In a previous study [Int. J. Mass Spectrom. 2010; 297: 67–75], the asymmetric O=U=O stretch (ν3) was measured for anionic uranyl complexes with composition [UO2(X)3]-, X = Cl-, Br- and I-. Within this group of complexes, the ν3 frequency red-shifts following the trend I > Br > Cl, suggesting concomitant weakening of the U=O bonds. However, a value for [UO2(F)3]- was not measured, which prevented a comprehensive comparison of measured ν3 positions to computed frequencies from density functional theory (DFT) calculations. Because the shift in ν3 is predicted to be most dramatic when X = F, we revisited these species using infrared multiple-photon photodissociation spectroscopy. As in our earlier study, a modest red-shift to the ν3 vibration of ∼ 6 cm-1 was observed for X = I-, Br-, and Cl-, and the position of the frequency follows the trend I- > Br- > Cl-. The value measured for [UO2(F)3]- is ∼43 cm-1 lower than the one measured for [UO2(Cl)3]-. Overall, the trend with respect to ν3 position is reproduced well by computed frequencies from DFT.

The gas-phase InfraRed Multiple Photon Dissociation (IRMPD) spectra in the fingerprint region of the anion (m/z 163) and mono-deprotonated homodimer of 9-methyl-guanine (2, m/z 329) and its d5 analogue (2-d5) are reported here. The anionic dimer is reverse Watson-Crick paired with the hydrogen bonding pattern ADD/DAA (where A stands for acceptor and D stands for donor), in which the site of negative charge is unambiguously found to be N1. The match between experimental vibrational spectra and DFT-computed spectra is good with the exception of the region between 2000 and 2900 cm-1 that contains symmetrical and antisymmetrical N-H stretches of the adjacent hydrogen-bond donor-donor pair.