Interface for a four-sector mass spectrometer with a dual-purpose collision cell: High transmission at low to intermediate energies

High-energy electron transfer dissociation (HE-ETD) using alkali metal targets for sequence analysis of post-translational peptides

Post-translational modifications (PTMs) of proteins are important in the activation, localization, and regulation of protein function in vivo. The usefulness of electron capture dissociation (ECD) and electron-transfer dissociation (ETD) in tandem mass spectrometry (MS/MS) using low-energy (LE) trap type mass spectrometer is associated with no loss of a labile PTM group regarding peptide and protein sequencing. The experimental results of high-energy (HE) collision induced dissociation (CID) using the Xe and Cs targets and LE-ETD were compared for doubly-phosphorylated peptides TGFLT(p)EY(p)VATR (1). Although HE-CID using the Xe target did not provide information on the amino acid sequence, HE-CID using the Cs target provided all the z-type ions without loss of the phosphate groups as a result of HE-ETD process, while LE-ETD using fluoranthene anion gave only z-type ions from z(5) to z(11). The difference in the results of HE-CID between the Xe and Cs targets demonstrated that HE-ETD process with the Cs target took place much more dominantly than collisional activation. The difference between HE-ETD using Cs targets and LE-ETD using the anion demonstrated that mass discrimination was much weaker in the high-energy process. HE-ETD was also applied to three other phosphopeptides YGGMHRQEX(p)VDC (2: X = S, 3: X = T, 4: X = Y). The HE-CID spectra of the doubly-protonated phosphopeptides (= [M + 2H](2+)) of 2, 3, and 4 using the Cs target showed a very similar feature that the c-type ions from c(7) to c(11) and the z-type ions from z(7) to z(11) were formed via N-C alpha bond cleavage without a loss of the phosphate group.

Energetics and Dynamics of Fragmentation of Protonated Leucine Enkephalin from Time- and Energy-Resolved Surface-Induced Dissociation Studies

Dissociation of singly protonated leucine enkephalin (YGGFL) was studied using surface-induced dissociation (SID) in a Fourier transform ion cyclotron resonance mass spectrometer (FT-ICR MS) specially configured for studying ion activation by collisions with surfaces. The energetics and dynamics of seven primary dissociation channels were deduced from modeling the time- and energy-resolved fragmentation efficiency curves for different fragment ions using an RRKM-based approach developed in our laboratory. The following threshold energies and activation entropies were determined in this study: E(0) = 1.20 eV and DeltaS++ = -20 eu(1) (MH(+)-->b(5)); E(0) = 1.14 eV and DeltaS++ = -14.7 eu (MH(+)-->b(4)); E(0) = 1.42 eV and DeltaS++ = -2.5 eu (MH(+)-->b(3)); E(0) = 1.30 eV and DeltaS++ = -4.1 eu (MH(+)-->a(4)); E(0) = 1.37 eV and DeltaS++ = -5.2 eu (MH(+)-->y ions); E(0) = 1.50 eV and DeltaS++ = 1.6 eu (MH(+)-->internal fragments); E(0) = 1.62 eV and DeltaS++ = 5.2 eu (MH(+)-->F). Comparison with Arrhenius activation energies reported in the literature demonstrated for the first time the reversal of the order of activation energies as compared to threshold energies for dissociation.

Mass analysis at the advent of the 21st century

There have been many new and exciting developments in mass spectrometer systems in recent years. Many of these developments are being driven by challenges presented by molecular biology. The activity is fueled by resources being devoted to drug development, for example, and other medically and biologically related activities. Progress in these applications will be accelerated by improved sensitivity, specificity, and speed. In mass spectrometry, this translates to greater mass resolving power, mass accuracy, mass-to-charge range, efficiency, and speed. It is safe to say that the demands resulting from current analytical needs are likely to be met to varying degrees but probably not by a single analyzer technology or hybrid instrument. On-line and/or off-line separations and manipulations combined with mass spectrometry will also play increasingly important roles. For any analyzer, or combination of analyzers, to become widely used it must have an important application for which its figures of merit are best suited, relative to competing approaches. The relative cost of competing technologies is also an important factor. The mass filter has seen so much use in the past 30 years because its characteristics best fit a wide range of applications. As an example, biological applications, which are currently driving many instrument development activities in mass spectrometry, demand more information, of higher quality, from less material, faster, and at lower cost. Which technologies will dominate biological applications in the coming years is open to speculation. However, in considering the relative merits of today's dominant mass analyzers, areas of opportunity for improvement are apparent. Furthermore, new and more demanding measurement needs are constantly being recognized that will continue to exercise the creativity of the mass spectrometry community.

Energy-resolved mass spectrometry: a comparison of quadrupole cell and cone-voltage collision-induced dissociation

Collision-induced dissociation (CID) can be effected in the interface region between atmospheric pressure ionization sources and single quadrupole mass analyzers. By varying the electric field in these cone-voltage CID experiments energy-resolved mass spectra can be obtained leading to breakdown graphs exploring the energy evolution of the fragmentation pathways. The breakdown graphs obtained from these cone-voltage CID studies are very comparable to those obtained by varying the collision energy in the quadrupole collision cell of a BEqQ mass spectrometer. The comparison has been made for the protonated peptides H-Leu-Gly-Gly-OH, H-Gly-Leu-Gly-OH, H-Gly-Gly-Leu-OH and Leu-enkephalin

The structure and fragmentation of B n (n≥3) ions in peptide spectra

The unimolecular and low energy collision-induced fragmentation reactions of the MH(+) ions of N-acetyl-tri-alanine, N-acetyl-tri-alanine methyl ester, N-acetyl-tetra-alanine, tetra-alanine, penta-alanine, hexa-glycine, and Leu-enkephalin have been studied with a particular emphasis on the formation and fragmentation of B n (n=3,4,5) ions. In addition, the metastable ion fragmentation reactions of protonated tetra-glycine, penta-glycine, and Leu-enkephalin amide have been studied. B n ions are prominent stable species in all spectra. The B n ions fragment, in part, by elimination of CO to form A n ions; this reaction occurs on the metastable ion time scale with a substantial release of kinetic energy (T 1/2=0. 3-0. 5 eV) that indicates that a stable configuration of the B n ion fragments by way of a reacting configuration that is higher in energy than the fragmentation products, A n + CO. Ab initio calculations strongly suggest that the stable configuration of the B3 and B4 ions is a protonated oxazolone formed by interaction of the developing charge with the next-nearest carbonyl group as HX is lost from the protonated species H-(Yyy) n -X · H(+). The higher B n ions also fragment, in part, to form the next-lower B ion, presumably in its stable protonated oxazolone form. This reaction is rationalized in terms of the three-dimensional structure of the B n ions and it is proposed that the neutral eliminated is an α-lactam.