Fragmentation of protonated oligoalanines: amide bond cleavage and beyond

Gas-phase fragmentation reactions of a7 ions containing a glutamine residue

The gas-phase fragmentation reactions of the a₇ ions derived from glutamine (Q) containing model heptapeptides have been studied in detail with low-energy collision-induced dissociation (CID) tandem mass spectrometry (MS/MS). Specifically, the positional effect of the Q residue has been investigated on the fragmentation reactions of a₇ ions. The study involves two sets of permuted isomers of the Q containing model heptapeptides. The first set contains the QAAAAAA sequence, and the second set involves of QYAGFLV sequence, where the position of the Q residue is changed from N- to C-terminal gradually for both peptide series. An intense loss of ammonia from the a7 ions followed by internal amino acid eliminations strongly supports forming the imine-amides structure via cyclization/rearrangement reaction for all studied a₇ ions. This is in agreement with the pioneering study reported by Bythell et al. (2010, 10.1021/ja101556g). A novel rearrangement reaction is detected upon fragmentation of imine-amide structure, which yields a protonated C-terminal amidated hexapeptide excluding the Q residue. A possible fragmentation mechanism was proposed to form the protonated C-terminal amidated hexapeptide, assisted via nucleophilic attack of the side chain amide nitrogen of the Q residue on its N-protonated imine carbon atom of the rearranged imine-amide structure. HIGHLIGHTS: The gas-phase fragmentation reactions of a₇ ions obtained from protonated model peptides containing glutamine residue were studied by ESI-MS/MS. A rearranged imine-amide structure is the predominant even for a₇ ions. Novel rearrangement reaction is observed which forms a protonated C-terminal amidated hexapeptide excluding Q residue upon fragmentation of the imine-amide structure.

Structures of a(n)* ions derived from protonated pentaglycine and pentaalanine: results from IRMPD spectroscopy and DFT calculations

Infrared multiple-photon dissociation (IRMPD) spectroscopy and DFT calculations have been used to probe the most stable structures of a3(*) and a4(*) ions derived from both protonated pentaglycine (denoted G5) and pentaalanine (A5). The a3(*) and a4(*) ions derived from protonated A5 feature a CHR=N-CHR'- group at the N-terminus and an oxazolone ring at the C-terminus, as proposed previously [J. Am. Soc. Mass Spectrom. 19, 1788-1798 (2008)]. The isomeric a4(*) ion derived from A5 with a 3,5-dihydro-4H-imidazol-4-one ring structure was calculated to have a slightly better energy than the oxazolone, but the barrier to its formation is higher and there was no evidence of this ion in the IRMPD spectrum. By contrast, the a4(*) and [a4 - H2O](+) (denoted a4(0)) ions from G5 gave strikingly similar IRMPD spectra and both have the 3,5-dihydro-4H-imidazol-4-one ring structure similar to that recently reported for the [GGGG + H - H2O](+) ion [Int. J. Mass Spectrom. 316-318, 268-272 (2012)]. In the absence of a solvent molecule, the pathway to the oxazolone is calculated to be lower than those to thermodynamically more stable products, the a4(0) and the a4(*) with the 3,5-dihydro-4H-imidazol-4-one ring structure. Incorporation of one water molecule is sufficient to reduce the barrier to formation of the a4(0) of G5 to below that for formation of the oxazolone. On the equivalent potential energy surface for protonated A5 the barrier to formation of the a4(0) ion is 12.3 kcal mol(-1) higher than that for oxazolone formation and the a4(0) ion is not observed experimentally.

Fragmentation reactions of methionine-containing protonated octapeptides and fragment ions therefrom: an energy-resolved study

The fragmentation reactions of the MH(+) ions as well as the b7, a7, and a7* ions derived therefrom have been studied in detail for the octapeptides MAAAAAAA, AAMAAAAA, AAAAMAAA, and AAAAAAMA. Ionization was by electrospray using a QqToF mass spectrometer, which allowed a study of the evolution of the fragmentation channels as a function of the collision energy. Not surprisingly, the product ion mass spectra for the b7 ions are independent of the original precursor sequence, indicating macrocyclization and reopening to the same mixture of protonated oxazolones prior to fragmentation. The results show that this sequence scrambling results in a distinct preference to place the Met residue in the C-terminal position of the protonated oxazolones. The a7 and a7* ions also produce product ion mass spectra independent of the original peptide sequence. The results for the a7 ions indicate that fragmentation occurs primarily from an amide structure analogous to that observed for a4 ions (Bythell et al. in J Am Chem Soc 132:14766-14779, 2010). Clearly, the rearrangement reaction they have proposed applies equally well to an ions as large as a7. The major fragmentation modes of the MH(+) ions at low collision energies produce b7, b6, and b5 ions. As the collision energy is increased further fragmentation of these primary products produces, in part, non-direct sequence ions, which become prominent at lower m/z values, particularly for the peptides with the Met residue near the N-terminus.

Using dissociation energies to predict observability of b- and y-peaks in mass spectra of short peptides. II. Results for hexapeptides with non-polar side chains

RATIONALE

The hypothesis that dissociation energies can serve as a predictor of observability of b- and y-peaks is tested for seven hexapeptides. If the hypothesis holds true for large classes of peptides, one would be able to improve the scoring accuracy of peptide identification tools by excluding theoretical peaks that cannot be observed in practical product ion spectra due to various physical, chemical or thermodynamic considerations.

METHODS

Product ion m/z spectra of hexapeptides AAAAAA, AAAFAA, AAAVAA, AAFAAA, AAVAAA, AAFFAA and AAVVAA have been acquired on a Finnigan LTQ XL mass spectrometer in the collision-induced dissociation (CID) activation mode on a grid of activation times 0.05 to 100 ms and normalized collision energy 10 to 35%. Dissociation energies were calculated for all fragmentation channels leading to b- and y-fragments at the TPSS/6-31G(d,p) level of the density functional theory.

RESULTS

It was demonstrated that the m/z peaks observed in the product ion spectra correspond to the fragmentation channels with dissociation energies below a certain threshold value. However, there is no direct correlation between the most intense m/z peaks and the lowest dissociation energies. Using the dissociation energies, it was predicted that out of 63 theoretically possible peaks in the b- and y-series of the seven hexapeptides, 19 should not be observable in practical spectra. In the experiments, 24 peaks were not observed, including all 19 predicted.

CONCLUSIONS

Dissociation energies alone are not sufficient for predicting ion intensity relationships in product ion m/z spectra. Nevertheless, the present data suggest that dissociation energies appear to be good predictors of observability of b- and y-peaks and potentially very useful for filtering theoretical peaks of each candidate peptide in peptide identification tools. Published 2012. This article is a US Government work and is in the public domain in the USA.

The influence glutamic acid in protonated b3 → b2 formation from VGEIG and related analogs

A direct pathway for the fragmentation of peptide b3 fragment ions to b2 ions has, until now, not been identified. Experimental evidence for the formation of a b3 anhydride structure and isomerization to an extended macrocycle is demonstrated here by comparison of the completely different fragmentation patterns of the b3 ions generated from protonated VGEIG and its methyl ester. In particular, the absence of a b2 ion in the fragmentation spectrum of the methyl ester b3 indicates that facile fragmentation of an anhydride-type b3 is responsible for virtually all b2 ions formed. The stability of this b3 structure and the ease with which it fragments to the b2 may be responsible for the relatively high abundance of the b3 and b2 ions. IRMPD action spectroscopy measurements indicate the presence of a ring protonated oxazolone in the b2 population. VGEIG and three related analogs, VALEIG, VADEIG, and V(Aib)EIG were studied by QCID-HDX-SORI experiments in an FT-ICR instrument, and provide significant evidence for extensive alpha proton scrambling in an ion-molecule complex formed between the b2 and neutral loss fragment following formation of the b2. MS3 and HDX of VG(2,2-d2)EIG indicate that the scrambled b2 ions have the same structure as the unscrambled b2. Based on these data and with the support of molecular modeling, we propose a new mechanism for this scrambling, in which the alpha protons are transferred in a multistep pathway during an ion-molecule complex formed between the b2 and amino-terminated anhydride ring neutral loss component.

Using dissociation energies to predict observability of b- and y-peaks in mass spectra of short peptides

RATIONALE

Peptide identification reliability can be improved by excluding from analysis those m/z peaks of candidate peptides which cannot be observed in practice due to various physical, chemical or thermodynamic considerations. We propose using dissociation energies (as opposed to proton affinities) as a predictor of observability of different m/z peaks in spectra of short peptides.

METHODS

Mass spectra of the tetrapeptides AAAA, AAFA, AAVA, AFAA, AVAA, AFFA, and AVVA were measured in the collision-induced dissociation (CID) activation mode on a grid of activation times 0.05 to 100 ms and normalized collision energy 10 to 35%. The lowest energy geometries and vibrational spectra were calculated for the precursor ions and their charged and neutral fragments using density functional theory (DFT) at the TPSS/6-31G(d,p) level. Dissociation energies were calculated for all fragmentation channels leading to b- or y-fragments.

RESULTS

It is demonstrated that m/z peaks observed in the mass spectra correspond to the fragmentation channels with the lowest dissociation energies. Using 50 kcal/mol as the cut-off value of dissociation energy, it was predicted that 28 out of 42 possible peaks in the b- and y-series of the seven tetrapeptides can be observed in mass spectra. In the experiments, 26 b- or y-peaks were observed, all of which are among the 28 predicted ones.

CONCLUSIONS

The use of dissociation energies generalizes the use of proton affinities for semi-quantitative predictions of relative intensities of different m/z peaks of short peptides. Further advances in this direction will pave the way for reliable quantitative predictions and, hence, for a significant improvement in robustness and accuracy of peptide and protein identification tools.

Influence of a Gamma Amino Acid on the Structures and Reactivity of Peptide a(3) Ions

Collision-induced dissociation of protonated AGabaAIG (where Gaba is gamma-amino butyric acid, NH(2)-(CH(2))(3)-COOH) leads to an unusually stable a(3) ion. Tandem mass spectrometry and theory are used here to probe the enhanced stability of this fragment, whose counterpart is not usually observed in CID of protonated peptides containing only alpha amino acids. Experiments are carried out on the unlabelled and (15)N-Ala labeled AGabaAIG (labeled separately at residue one or three) probing the b(3), a(3), a(3)-NH(3) (a(3) (*)), and b(2) fragments while theory is used to characterize the most stable b(3), a(3), and b(2) structures and the formation and dissociation of the a(3) ion. Our results indicate the AGabaA oxazolone b(3) isomer undergoes head-to-tail macrocyclization and subsequent ring opening to form the GabaAA sequence isomer while this chemistry is energetically disfavored for the AAA sequence. The AGabaA a(3) fragment also undergoes macrocyclization and rearrangement to form the rearranged imine-amide isomer while this reaction is energetically disfavored for the AAA sequence. The barriers to dissociation of the AGabaA a(3) ion via the a(3)→b(2) and a(3)→a(3)* channels are higher than the literature values reported for the AAA sequence. These two effects provide a clear explanation for the enhanced stability of the AGabaA a(3) ion.

Electrospray ionization mass spectrometry: a technique to access the information beyond the molecular weight of the analyte

The Electrospray Ionization (ESI) is a soft ionization technique extensively used for production of gas phase ions (without fragmentation) of thermally labile large supramolecules. In the present review we have described the development of Electrospray Ionization mass spectrometry (ESI-MS) during the last 25 years in the study of various properties of different types of biological molecules. There have been extensive studies on the mechanism of formation of charged gaseous species by the ESI. Several groups have investigated the origin and implications of the multiple charge states of proteins observed in the ESI-mass spectra of the proteins. The charged analytes produced by ESI can be fragmented by activating them in the gas-phase, and thus tandem mass spectrometry has been developed, which provides very important insights on the structural properties of the molecule. The review will highlight recent developments and emerging directions in this fascinating area of research.

N-Protonated isomers as gateways to peptide ion fragmentation

According to the popular "mobile proton model" for peptide ion fragmentation in tandem mass spectrometry, peptide bond cleavage is typically preceded by intramolecular proton transfer from basic sites to an amide nitrogen in the backbone. If the intrinsic barrier to dissociation is the same for all backbone sites, the fragmentation propensity at each amide bond should reflect the stability of the corresponding N-protonated isomer. This hypothesis was tested by using ab initio and force-field computations on several polyalanines and Leu-enkephalin. The results agree acceptably with experimental reports, supporting the hypothesis. It was found that backbone N-protonation is most favorable near the C-terminus. The preference for C-terminal N-protonation, which is stronger for longer polyalanines, may be understood in terms of the well known "helix macrodipole" in the corresponding helical conformations. The opposite stability trend is found for peptides constrained to be linear, which is initially surprising but turns out to be consistent with the reversed direction of the macrodipole in the linear conformation.

Fragmentation characteristics of b(n) (n=2-15) ions from protonated peptides

The fragmentation reactions of protonated oligoalanines (trialanine, tetraalanine and pentaalanine) and the fragments present in the electrospray ionization (ESI) mass spectrum of polyalanine have been studied by collisionally activated dissociation (CAD) mass spectrometry (MS(2) and MS(3) experiments). The MS(n) experiments provided strong evidence that the m/z 71n+1 ion series in the ESI mass spectrum of polyalanine is a b(n) series. These ions are formed via the b(n) -y(m) pathway of amide bond cleavage, which results in the formation of a proton-bound complex of an oxazolone and a peptide/amino acid. Also, the MS(2) spectra of the b(n) series from polyalanine revealed that the chain length of b(n) ions influences significantly the dissociations taking place. For example, b(n) ions start losing H(2)O at n ≥5 and the losses of CO and CO+NH(3) decrease in intensity from b(2) to b(15). The elimination of H(2)O+NH(3) and the elimination of 61 mass (HN=C=O+H(2)O) commence with b(6); their abundances initially increase up to ~ b(8)-b(9) and then gradually decrease until b(15) (largest fragment studied). The tandem mass spectrometry experiments help to elucidate the dissociation mechanisms of the observed structures of biopolymer fragments.

Towards understanding the tandem mass spectra of protonated oligopeptides. 2: The proline effect in collision-induced dissociation of protonated Ala-Ala-Xxx-Pro-Ala (Xxx = Ala, Ser, Leu, Val, Phe, and Trp)

The product ion spectra of proline-containing peptides are commonly dominated by y(n) ions generated by cleavage at the N-terminal side of proline residues. This proline effect is investigated in the current work by collision-induced dissociation (CID) of protonated Ala-Ala-Xxx-Pro-Ala (Xxx includes Ala, Ser, Leu, Val, Phe, and Trp) in an electrospray/quadrupole/time-of-flight (QqTOF) mass spectrometer and by quantum chemical calculations on protonated Ala-Ala-Ala-Pro-Ala. The CID spectra of all investigated peptides show a dominant y(2) ion (Pro-Ala sequence). Our computational results show that the proline effect mainly arises from the particularly low threshold energy for the amide bond cleavage N-terminal to the proline residue, and from the high proton affinity of the proline-containing C-terminal fragment produced by this cleavage. These theoretical results are qualitatively supported by the experimentally observed y(2)/b(3) abundance ratios for protonated Ala-Ala-Xxx-Pro-Ala (Xxx = Ala, Ser, Leu, Val, Phe, and Trp). In the post-cleavage phase of fragmentation the N-terminal oxazolone fragment with the Ala-Ala-Xxx sequence and Pro-Ala compete for the ionizing proton for these peptides. As the proton affinity of the oxazolone fragment increases, the y(2)/b(3) abundance ratio decreases.

Studies of gas-phase reactions of cationic iron complexes of 2-pyrimidinyloxy-N-arylbenzylamines by electrospray ionization tandem mass spectrometry

Electrospray ionization triple quadrupole mass spectrometry (ESI-TSQ-MS) and electrospray ionization Fourier transform ion cyclotron resonance mass spectrometry (ESI-FTICR-MS) were used to investigate the interesting gas-phase reactions of the cationic iron (Fe) complexes of 2-pyrimidinyloxy-N-arylbenzylamines (1-6), which are generated by ESI when mixing their methanolic solutions. Further studies of these Fe complexes by collision-induced dissociation (CID) show that Fe(III) complexes undergo an interesting gas-phase single electron transfer (SET) reaction to give 1(•+) -6(•+) ,with loss of neutral FeCl(2) , whereas Fe(II) can catalyze gas-phase Smiles rearrangement reactions of compounds 1-6. By using different Fe(II)X(2) salts (X = Cl or Br) with a set of reactants, the role of the counterion (X(-) ) and the structure effect of the reactants on Fe(II)-catalyzed gas-phase Smiles rearrangement reactions are studied. Evidence obtained from by TSQ-MS and FTICR-MS experiments, hydrogen/deuterium (H/D) exchange experiments and theoretical computations supported some unique gas-phase chemistries initiated by introduction of Fe(II) into 1. Importantly, by comparing the distinct gas-phase reaction results of the cationic Fe(III) complexes with those of Fe(II) complexes, the charge state effects of iron on the gas-phase chemistries of Fe complexes are revealed.

The extent and effects of peptide sequence scrambling via formation of macrocyclic B ions in model proteins

The extent and effects of sequence scrambling in peptide ions during tandem mass spectrometry (MS/MS) have been examined using tryptic peptides from model proteins. Sequence-scrambled b ions appeared in about 35% of 43 tryptic peptides examined under MS/MS conditions. In general, these ions had relatively low abundances with averages of 8% and 16%, depending on the instrumentation used. A few tryptic peptides gave abundant scrambled b ions in MS/MS. However, peptide and protein identifications under proteomic conditions with Mascot were not affected, even for these peptides wherein scrambling was prominent. From the 43 tryptic peptides that have been investigated, the conclusion is that sequence scrambling is unlikely to impact negatively on the accuracy of automated peptide and protein identifications in proteomics.

Effect of the His residue on the cyclization of b ions

The MS(n) spectra of the [M + H](+) and b(5) peaks derived from the peptides HAAAAA, AHAAAA, AAHAAA, AAAHAA, and AAAAHA have been measured, as have the spectra of the b(4) ions derived from the first four peptides. The MS(2) spectra of the [M + H](+) ions show a substantial series of b(n) ions with enhanced cleavage at the amide bond C-terminal to His and substantial cleavage at the amide bond N-terminal to His (when there are at least two residues N-terminal to the His residue). There is compelling experimental and theoretical evidence for formation of nondirect sequence ions via cyclization/reopening chemistry in the CID spectra of the b ions when the His residue is near the C-terminus. The experimental evidence is less clear for ions when the His residue is near the N-terminus, although this may be due to the use of multiple alanine residues in the peptide making identifying scrambled peaks more difficult. The product ion mass spectra of the b(4) and b(5) ions from these isomeric peptides with cyclically permuted amino acid sequences are similar, but also show clear differences. This indicates less active cyclization/reopening followed by fragmentation of common structures for b(n) ions containing His than for sequences of solely aliphatic residues. Despite more energetically favorable cyclization barriers for the b(5) structures, the b(4) ions experimental data show more clear evidence of cyclization and sequence scrambling before fragmentation. For both b(4) and b(5) the energetically most favored structure is a macrocyclic isomer protonated at the His side chain.

Gas-phase acidities of cysteine-polyglycine peptides: the effect of the cysteine position

The sequence and conformational effects on the gas-phase acidities of peptides have been studied by using two pairs of isomeric cysteine-polyglycine peptides, CysGly(3,4)NH(2) and Gly(3,4)CysNH(2). The extended Cooks kinetic method was employed to determine the gas-phase acidities using a triple quadrupole mass spectrometer with an electrospray ionization source. The ion activation was achieved via collision-induced dissociation experiments. The deprotonation enthalpies (Delta(acid)H) were determined to be 323.9 +/- 2.5 kcal/mol (CysGly(3)NH(2)), 319.2 +/- 2.3 kcal/mol (CysGly(4)NH(2)), 333.8 +/- 2.1 kcal/mol (Gly(3)CysNH(2)), and 321.9 +/- 2.8 kcal/mol (Gly(4)CysNH(2)), respectively. The corresponding deprotonation entropies (Delta(acid)S) of the peptides were estimated. The gas-phase acidities (Delta(acid)G) were derived to be 318.4 +/- 2.5 kcal/mol (CysGly(3)NH(2)), 314.9 +/- 2.3 kcal/mol (CysGly(4)NH(2)), 327.5 +/- 2.1 kcal/mol (Gly(3)CysNH(2)), and 317.4 +/- 2.8 kcal/mol (Gly(4)CysNH(2)), respectively. Conformations and energetic information of the neutral and anionic peptides were calculated through simulated annealing (Tripos), geometry optimization (AM1), and single point energy calculations (B3LYP/6-31+G(d)), respectively. Both neutral and deprotonated peptides adopt many possible conformations of similar energies. All neutral peptides are mainly random coils. The two C-cysteine anionic peptides, Gly(3,4)(Cys-H)(-)NH(2), are also random coils. The two N-cysteine anionic peptides, (Cys-H)(-)Gly(3,4)NH(2), may exist in both random coils and stretched helices. The two N-cysteine peptides, CysGly(3)NH(2) and CysGly(4)NH(2), are significantly more acidic than the corresponding C-terminal cysteine ones, Gly(3)CysNH(2) and Gly(4)CysNH(2). The stronger acidities of the former may come from the greater stability of the thiolate anion resulting from the interaction with the helix-macrodipole, in addition to the hydrogen bonding interactions.

Charge-separation reactions of doubly-protonated peptides: effect of peptide chain length

The collision induced dissociation of doubly-protonated (Ala)(x)His (x = 5, 6, 7, 8, 10) peptides have been studied. The major fragmentation reactions observed are symmetrical amide bond cleavages to give the complementary b(m) and y(N-m) ions, where N is the total number of residues in the peptide. Minor asymmetric cleavage to give doubly-protonated y ions also is observed, involving cleavage near the N-terminus. The shorter peptides (x = 5, 6, 7) show major cleavage of the second amide bond to yield b2 and y(N-2) ions, while (Ala)10His shows major symmetrical cleavage at the fourth and fifth amide bonds. (Ala)8His appears to be a transitional peptide in showing substantial symmetrical cleavage at the second, fourth, and fifth amide bonds. The results are in general agreement with the bifurcating nature of charge separation noted by Zubarev (J. Am. Soc. Mass Spectrom.2008, 19, 1755-1763) from a statistical analysis of a large body of doubly-protonated tryptic peptide CID mass spectra. It is shown that the b2 ion derived from doubly-protonated (Ala)5His has a protonated oxazolone structure.

To b or not to b: the ongoing saga of peptide b ions

Modern soft ionization techniques readily produce protonated or multiply protonated peptides. Collision-induced dissociation (CID) of these protonated species is often used as a method to obtain sequence information. In many cases fragmentation occurs at amide bonds. When the charge resides on the C-terminal fragment so-called y ions are produced which are known to be protonated amino acids or truncated peptides. When the charge resides on the N-terminal fragment so-called b ions are produced. Often the sequence of y and b ions are essential for peptide sequencing. The b ions have many possible structures, a knowledge of which is useful in this sequencing. The structures of b ions are reviewed in the following with particular emphasis on the variation of structure with the number of amino acid residues in the b ion and the effect of peptide side chain on b ion structure. The recent discovery of full cyclization of larger b ions results in challenges in peptide sequencing. This aspect is discussed in detail.

Fragmentation reactions of some peptide b3 ions: an energy-resolved study

The fragmentation reactions of b3 ions of nominal structure AAAoxa, YAAoxa, AYAoxa and AAYoxa have been studied as a function of collision energy, allowing the construction of breakdown graphs expressing in a qualitative way the energy dependence of the fragmentation reactions. The primary fragmentation reactions of the AAAoxa b3 ion involve formation of the a3* (a3-NH3) ion and the b2 ion, with the latter becoming the dominant product at higher internal energies. For both YAAoxa and AYAoxa b3 ions the pathway to a3* is relatively minor with formation of b2 the dominant primary fragmentation reaction. For the AAYoxa b3 ion, in addition to a3*, abundant formation of the tyrosine (Y) iminium ion is observed with only minor formation of the b2 ion. The results support and expand upon the detailed mechanism of fragmentation of b3 ions proposed by Cooper et al. (J. Am. Soc. Mass Spectrom. 2006; 17: 1654).

Structure and reactivity of a(n) and a(n) peptide fragments investigated using isotope labeling, tandem mass spectrometry, and density functional theory calculations

Extensive (15)N labeling and multiple-stage tandem mass spectrometry were used to investigate the fragmentation pathways of the model peptide FGGFL during low-energy collision-induced-dissociation (CID) in an ion-trap mass spectrometer. Of particular interest was formation of a(4) from b(4) and a(4) (a(4)-NH(3)) from a(4) ions correspondingly, and apparent rearrangement and scrambling of peptide sequence during CID. It is suggested that the original FGGF(oxa)b(4) structure undergoes b-type scrambling to form GGFF(oxa). These two isomers fragment further by elimination of CO and (14)NH(3) or (15)NH(3) to form the corresponding a(4)and a(4) isomers, respectively. For ((15)N-F)GGFL and FGG((15)N-F)L the a(4) ion population appears as two distinct peaks separated by 1 mass unit. These two peaks could be separated and fragmented individually in subsequent CID stages to provide a useful tool for exploration of potential mechanisms along the a(4) --> a(4) pathway reported previously in the literature (Vachet et al. J. Am. Chem. Soc.1997, 119, 5481, and Cooper et al. J. Am. Soc. Mass Spectrom.2006, 17, 1654). These mechanisms result in formally the same a(4) structures but differ in the position of the expelled nitrogen atom. Detailed analysis of the observed fragmentation patterns for the separated light and heavy a(4) ion fractions of ((15)N-F)GGFL indicates that the mechanism proposed by Cooper et al. is consistent with the experimental findings, while the mechanism proposed by Vachet et al. cannot account for the labeling data. In addition, a new rearrangement pathway is presented for a(4)-CO ions that effectively transfers the former C-terminal amino acid residue to the N-terminus.

Peptide sequence scrambling through cyclization of b(5) ions

The CID mass spectra of the MH(+) ions and the b(5) ions derived therefrom have been determined for the hexapeptides YAAAAA, AYAAAA, AAYAAA, AAAYAA, and AAAAYA. The CID mass spectra for the b(5) ions derived from the five isomers are essentially identical and show abundant ion signals for nonsequence b ions. This result is consistent with cyclization of the b(5) ions to a cyclic pentapeptide before fragmentation; this cyclic peptide can open at various positions, leading to losses of amino acid residues that are not characteristic of the original amino acid sequence. These nonsequence b ions are also observed in the fragmentation of the MH(+) ions and increase substantially in importance with increasing collision energy. A comparison of the fragmentation of AAAYAA and Ac-AAAYAA indicates that N-acetylation eliminates the cyclization of b(5) ions and, thus, eliminates the nonsequence ions in the CID mass spectra of both b(5) and MH(+) ions.

Infrared Spectroscopy and Theoretical Studies on Gas-Phase Protonated Leu-enkephalin and Its Fragments: Direct Experimental Evidence for the Mobile Proton

The gas-phase structures of the protonated pentapeptide Leu-enkephalin and its main collision-induced dissociation (CID) product ions, b4 and a4, are investigated by means of infrared multiple-photon dissociation (IR-MPD) spectroscopy and detailed molecular mechanics and density functional theory (DFT) calculations. Our combined experimental and theoretical approach allows accurate structural probing of the site of protonation and the rearrangement reactions that have taken place in CID. It is shown that the singly protonated Leu-enkephalin precursor is protonated on the N-terminus. The b4 fragment ion forms two types of structures: linear isomers with a C-terminal oxazolone ring, as well as cyclic peptide structures. For the former structure, two sites of proton attachment are observed, on the N-terminus and on the oxazolone ring nitrogen, as shown in a previous communication (Polfer, N. C.; Oomens, J.; Suhai, S.; Paizs, B. J. Am. Chem. Soc. 2005, 127, 17154-17155). Upon leaving the ions for longer radiative cooling delays in the ion cyclotron resonance (ICR) cell prior to IR spectroscopic investigation, one observes a gradual decrease in the relative population of oxazolone-protonated b4 and a corresponding increase in N-terminal-protonated b4. This experimentally demonstrates that the mobile proton is transferred between two sites in a gas-phase peptide ion and allows one to rationalize how the proton moves around the molecule in the dissociation process. The a4 fragment, which is predominantly formed via b4, is also confirmed to adopt two types of structures: linear imine-type structures, and cyclic structures; the former isomers are exclusively protonated on the N-terminus in sharp contrast to b4, where a mixture of protonation sites was found. The presence of cyclic b4 and a4 fragment ions is the first direct experimental proof that fully cyclic structures are formed in CID. These results suggest that their presence is significant, thus lending strong support to the recently discovered peptide fragmentation pathways (Harrison, A. G.; Young, A. B.; Bleiholder, B.; Suhai, S.; Paizs, B. J. Am. Chem. Soc. 2006, 128, 10364-10365) that result in scrambling of the amino acid sequence upon CID.

Cyclization reaction of peptide fragment ions during multistage collisionally activated decomposition: an inducement to lose internal amino-acid residues

During characterization of some peptides (linear precursors of the cyclic peptides showing potential to be anticancer drugs) in an ion trap, it was noted that many internal amino acid residues could be lost from singly charged b ions. The phenomenon was not obvious at the first stage of collisionally activated decomposition (CAD), but was apparent at multiple stages of CAD. The unique fragmentation consisting of multiple steps is induced by a cyclization reaction of b ions, the mechanism of which has been probed by experiments of N-acetylation, MS(n), rearranged-ion design, and activation-time adjustment. The fragmentation of synthetic cyclic peptides demonstrates that a cyclic peptide intermediate (CPI) formed by b ion cyclization exhibits the same fragmentation pattern as a protonated cyclic peptide. Although no rules for the cyclization reaction were discerned in the experiments of peptide modification, the fragmentations of a number of b ions indicate that the "Pro and Asn/Gln effects" can influence ring openings of CPIs. In addition, large-scale losses of internal residues from different positions of a-type ions have been observed when pure helium was used as collision gas. The fragmentation is initiated by a cyclization reaction forming an a-type ion CPI. This CPI with a fixed-charge structure cannot be influenced by the "Pro effect", causing a selective ring opening at the amide bond Pro-Xxx rather than Xxx-Pro. With the knowledge of the unique fragmentations leading to internal residue losses, the misidentification of fragments and sequences of peptides may be avoided.

Dehydration versus deamination of N-terminal glutamine in collision-induced dissociation of protonated peptides

Some of the most prominent "neutral losses" in peptide ion fragmentation are the loss of ammonia and water from N-terminal glutamine. These processes are studied by electrospray ionization mass spectrometry in singly- and doubly-protonated peptide ions undergoing collision-induced dissociation in a triple quadrupole and in an ion trap instrument. For this study, four sets of peptides were synthesized: (1) QLLLPLLLK and similar peptides with K replaced by R, H, or L, and Q replaced by a number of amino acids, (2) QLnK (n = 0, 1, 3, 5, 7, 9, 11), (3) QLnR (n = 0, 1, 3, 5, 7, 9), and (4) QLn (n = 1, 2, 3, 4, 8). The results for QLLLPLLLK and QLLLPLLLR show that the singly protonated ions undergo loss of ammonia and to a smaller extent loss of water, whereas the doubly protonated ions undergo predominant loss of water. The fast fragmentation next to P (forming the y5 ion) occurs to a larger extent than the neutral losses from the singly protonated ions but much less than the water loss from the doubly protonated ions. The results from these and other peptides show that, in general, when N-terminal glutamine peptides have no "mobile protons", that is, the number of charges on the peptide is no greater than the number of basic amino acids (K, R, H), deamination is the predominant neutral loss fragmentation, but when mobile protons are present the predominant process is the loss of water. Both of these processes are faster than backbone fragmentation at the proline. These results are rationalized on the basis of resonance stabilization of the two types of five-membered ring products that would be formed in the neutral loss processes; the singly protonated ion yields the more stable neutral pyrrolidinone ring whereas the doubly protonated ion yields the protonated aminopyrroline ring (see Schemes). The generality of these trends is confirmed by analyzing an MS/MS spectra library of peptides derived from tryptic digests of yeast. In the absence of mobile protons, glutamine deamination is the most rapid neutral loss process. For peptides with mobile protons, dehydration from glutamine is far more rapid than from any other amino acid. Most strikingly, end terminal glutamine is by far the most labile source of neutral loss in excess-proton peptides, but not highly exceptional when mobile protons are not available. In addition, rates of deamination are faster in lysine versus arginine C-terminus peptides and 20 times faster in positively charged than negatively charged peptides, demonstrating that these formal neutral loss reactions are not "neutral reactions" but depend on charge state and stability.

Isotope labeling and theoretical study of the formation of a3* ions from protonated tetraglycine

Extensive 13C, 15N, and 2H labeling of tetraglycine was used to investigate the b3+ --> a3* reaction during low-energy collision-induced dissociation (CID) in a quadrupole ion-trap mass spectrometer. The patterns observed with respect to the retention or elimination of the isotope labels demonstrate that the reaction pathway involves elimination of CO and NH3. The ammonia molecule includes 2 H atoms from amide or amino positions, and one from an alpha-carbon position. The loss of NH3 does not involve elimination of the N-terminal amino group but, instead, the N atom of the presumed oxazolone ring in the b3+ ion. The CO molecule eliminated is the carbonyl group of the same oxazolone ring, and the alpha-carbon H atom is transferred from the amino acid adjacent to the oxazolone ring. Quantum chemical calculations indicate a multistep reaction cascade involving CO loss on the b3 --> a3 pathway and loss of NH=CH2 from the a3 ion to form b2. In the postreaction complex of b2 and NH=CH2, the latter can be attacked by the N-terminal amino group of the former. The product of this attack, an isomerized a3 ion, can eliminate NH3 from its N-terminus to form a3*. Calculations suggest that the ammonia and a3* species can form various ion-molecule complexes, and NH3 can initiate relay-type mobilization of the oxazolone H atoms from alpha-carbon positions to form a new oxazolone isomer. This multiple-step reaction scheme clearly explains the isotope labeling results, including unexpected scrambling of H atoms from alpha-carbon positions.

Revising the proton affinity scale of the naturally occurring alpha-amino acids

The proton affinities (PA) of the 20 naturally occurring alpha-amino acids (AA) have been determined computationally by means of density functional theory (DFT) and high-level G2(MP2) calculations. These theoretical PAs, together with data that have appeared since 1997 in the literature, are used to validate the most reasonable currently available PA scale for AAs (Harrison, A. G. Mass Spectrom. Rev. 1997, 16, 201-217.). Significant scatter is observed for the PAs of Ser, Asp, Phe, Asn, Met, Pro, Gln, Glu, Trp, His, Lys, and Arg, many of which have a basic side-chain functionality. Critical review of the available data leads to new consensus PAs for Asn, Gln, Met, and Arg of 222.4, 230.5, 223.7, and 250.2 kcal/mol, respectively.

Collision-induced dissociation of protonated tetrapeptides containing beta-alanine, gamma-aminobutyric acid, epsilon-aminocaproic acid or 4-aminomethylbenzoic acid residues

The influence of the presence and position of a single beta-alanine, gamma-aminobutyric acid, epsilon-aminocaproic acid or 4-aminomethylbenzoic acid residue on the tendency to form b(n)+ -and y(n)+ -type product ions was determined using a group of protonated tetrapeptides with general sequence XAAG, AXAG and AAXG (where X refers to the position of amino acid substitution). The hypothesis tested was that the 'alternative' amino acids would influence product ion signal intensities by inhibiting or suppressing either the nucleophilic attack or key proton transfer steps by forcing the adoption of large cyclic intermediates or blocking cyclization altogether. We found that specific b ions are diminished or eliminated completely when betaA, gammaAbu, Cap or 4AMBz residues are positioned such that they should interfere with the intramolecular nucleophilic attack step. In addition, differences in the relative proton affinities of the alternative amino acids influence the competition between complementary b(n) and y(n) ions. For both the AXAG and the XAAG series of peptides, collision-induced dissociation (CID) generated prominent b ions despite potential inhibition or suppression of intramolecular proton migration by the betaA, gammaAbu, Cap or 4AMBz residues. The prominent appearance of b ions from the AXAG and XAAG peptide is noteworthy, and suggests either that proton migration occurs through larger, 'whole' peptide cyclic intermediates or that fragmentation proceeds through a population of [M+H]+ isomers that are initially protonated at amide O atoms.

Mass spectrometric studies of the gas phase retro-Michael type fragmentation reactions of 2-hydroxybenzyl-N-pyrimidinylamine derivatives

The gas-phase fragmentation reactions of 2-hydroxybenzyl-N-pyrimidinylamine derivatives (Compounds 1 to 6), the O-N-type acid-catalyzed Smiles rearrangement products of 2-pyrimidinyloxy-N-arylbenzylamine derivatives, have been examined via positive ion matrix-assisted laser desorption/ionization (MALDI) infrared multiphoton dissociation (IRMPD) mass spectrometry in FT-ICR MS and via negative ion electrospray ionization (ESI) in-source collision-induced dissociation (CID) mass spectrometry, respectively. The major fragmentation pathway of protonated 1 to 6 gives the F ions under IRMPD; theoretical results show that the retro-Michael reaction channel is more favorable in both thermodynamics and kinetics. This explanation is supported by H/D exchange experiments and the MS/MS experiment of acetylated 1. Deprotonated 1 to 6 give rise to the solitary E ions (aromatic nitrogen anions) in the negative ion in-source CID; theoretical calculations show that a retro-Michael mechanism is more reasonable than a gas-phase intramolecular nucleophilic displacement (SN2) mechanism to explain this reaction process.