Mass accuracy is a key parameter of mass spectrometric performance. TOF instruments can reach low parts per million, and FT-ICR instruments are capable of even greater accuracy provided ion numbers are well controlled. Here we demonstrate sub-ppm mass accuracy on a linear ion trap coupled via a radio frequency-only storage trap (C-trap) to the orbitrap mass spectrometer (LTQ Orbitrap). Prior to acquisition of a spectrum, a background ion originating from ambient air is first transferred to the C-trap. Ions forming the MS or MSn spectrum are then added to this species, and all ions are injected into the orbitrap for analysis. Real time recalibration on the “lock mass” by corrections of mass shift removes mass error associated with calibration of the mass scale. The remaining mass error is mainly due to imperfect peaks caused by weak signals and is addressed by averaging the mass measurement over the LC peak, weighted by signal intensity. For peptide database searches in proteomics, we introduce a variable mass tolerance and achieve average absolute mass deviations of 0.48 ppm (standard deviation 0.38 ppm) and maximal deviations of less than 2 ppm. For tandem mass spectra we demonstrate similarly high mass accuracy and discuss its impact on database searching. High and routine mass accuracy in a compact instrument will dramatically improve certainty of peptide and small molecule identification. Mass accuracy is a key parameter of mass spectrometric performance. TOF instruments can reach low parts per million, and FT-ICR instruments are capable of even greater accuracy provided ion numbers are well controlled. Here we demonstrate sub-ppm mass accuracy on a linear ion trap coupled via a radio frequency-only storage trap (C-trap) to the orbitrap mass spectrometer (LTQ Orbitrap). Prior to acquisition of a spectrum, a background ion originating from ambient air is first transferred to the C-trap. Ions forming the MS or MSn spectrum are then added to this species, and all ions are injected into the orbitrap for analysis. Real time recalibration on the “lock mass” by corrections of mass shift removes mass error associated with calibration of the mass scale. The remaining mass error is mainly due to imperfect peaks caused by weak signals and is addressed by averaging the mass measurement over the LC peak, weighted by signal intensity. For peptide database searches in proteomics, we introduce a variable mass tolerance and achieve average absolute mass deviations of 0.48 ppm (standard deviation 0.38 ppm) and maximal deviations of less than 2 ppm. For tandem mass spectra we demonstrate similarly high mass accuracy and discuss its impact on database searching. High and routine mass accuracy in a compact instrument will dramatically improve certainty of peptide and small molecule identification. The data produced by a mass spectrometer are the mass and intensity of compounds and their fragments. The accuracy of mass measurement directly determines the usefulness of mass spectrometric experiments, and much effort in instrumentation development is directed at improving this key parameter. Mass accuracy and mass resolution are connected, and instruments introduced during the last decades radically improved in these two attributes. Traditionally accurate mass measurements, sufficient to determine the elemental composition of small molecules, were the province of magnetic sector instruments, but today TOF instruments equipped with energy correcting reflectrons can reach low ppm values. Triple quadrupole instruments or quadrupole ion traps, which are popular in proteomics research, however, have low resolution and mass uncertainties of typically half to several Da. At the other extreme, FT-ICR mass spectrometers reduce the mass measurement to a frequency measurement and are therefore potentially capable of exceedingly high mass accuracy. In practice, however, FT-ICR instruments have suffered from the requirement to precisely control the number of ions accumulated in the Penning trap. Over or under filling leads to mass shifts to high and low values, respectively. For example, Smith and co-workers (1Belov M.E. Zhang R. Strittmatter E.F. Prior D.C. Tang K. Smith R.D. Automated gain control and internal calibration with external ion accumulation capillary liquid chromatography-electrospray ionization Fourier transform ion cyclotron resonance.Anal. Chem. 2003; 75: 4195-4205Google Scholar) reported that in their measurements the mass determined over an LC peak varied by more than 10 ppm. The recent introduction of a linear ion trap-FT-ICR combination (2Syka J.E.P. Marto J.A. Bai D.L. Horning S. Senko M.W. Schwartz J.C. Ueberheide B. Garcia B. Busby S. Muratore T. Shabanowitz J. Hunt D.F. Novel Linear Quadrupole Ion Trap/FT Mass Spectrometer: Performance Characterization and Use in the Comparative Analysis of Histone H3 Post-translational Modifications.J. Proteome Res. 2004; 3: 621-626Google Scholar) largely solved this problem through a prescan in the ion trap to estimate ion current (called automatic gain control), which allows filling of the ICR cell with a predetermined number of ions. Using automatic gain control and narrow mass ranges (SIM 1The abbreviations used are: SIM, selected ion monitoring; MS/MS, tandem MS; LTQ, Thermo Electron linear quadrupole ion trap; RF, radio frequency; SILAC, stable isotope labeling by amino acids in cell culture; PCM, polycyclodimethylsiloxane. scans) we observed an average absolute mass error between 0.6 and 0.7 ppm in recent large scale proteomic analyses (3Olsen J.V. Ong S.E. Mann M. Trypsin cleaves exclusively C-terminal to arginine and lysine residues.Mol. Cell Proteomics. 2004; 3: 608-614Google Scholar, 4Andersen J.S. Lam Y.W. Leung A.K. Ong S.E. Lyon C.E. Lamond A.I. Mann M. Nucleolar proteome dynamics.Nature. 2005; 433: 77-83Google Scholar, 5Gruhler A. Olsen J.V. Mohammed S. Mortensen P. Faergeman N.J. Mann M. Jensen O.N. Quantitative phosphoproteomics applied to the yeast pheromone signaling pathway.Mol. Cell Proteomics. 2005; 4: 310-327Google Scholar). In a typical proteomics experiment, protein mixtures are digested to peptide mixtures that are separated by reversed phase HPLC and analyzed on-line by MS and MS/MS (6Aebersold R. Mann M. Mass spectrometry-based proteomics.Nature. 2003; 422: 198-207Google Scholar). The mass accuracy achieved in the instrument directly translates into the mass tolerances that can be specified in subsequent database searches of tandem mass spectra. Unambiguous protein identification in large data sets is by no means trivial (7Steen H. Mann M. The abc’s (and xyz’s) of peptide sequencing.Nat. Rev. Mol. Cell. Biol. 2004; 5: 699-711Google Scholar), and any increase in achieved mass accuracy greatly aids the specificity of database searches in two ways (8Jensen O.N. Podtelejnikov A. Mann M. Delayed Extraction Improves Specificity in Database Searches by MALDI Peptide Maps.Rapid Commun. Mass Spectrom. 1996; 10: 1371-1378Google Scholar, 9Clauser K.R. Baker P. Burlingame A.L. Role of accurate mass measurement (+/− 10 ppm) in protein identification strategies employing MS or MS/MS and database searching.Anal. Chem. 1999; 71: 2871-2882Google Scholar): High precursor mass accuracy in the MS spectra directly translates into fewer “candidate sequences” that need to be considered as possible matches. High mass accuracy in the MS/MS spectra leads to fewer measured fragment masses that match the calculated fragments of a candidate sequence by chance and therefore decreases the scores of false positives in database search algorithms. In 1923, Kingdon (10Kingdon K. A method for the neutralization of electron space charge by positive ionization at very low gas pressures.Phys. Rev. 1923; 21: 408-418Google Scholar) devised a method to capture ions by causing them to orbit around a central electrode. Since then, the physics community has used “Kingdon traps” in a variety of experiments, but it was always used as a capturing device, not as a mass spectrometer. A few years ago a mass which the orbitrap A. a of mass Chem. Scholar, M. A. the orbitrap mass to an ion Chem. 2003; 75: Scholar, H. A. M. R. The a mass Mass Spectrom. 2005; Scholar). the of this a mass spectrometer was very introduced of the linear ion trap coupled to a radio frequency for storage of ions and of the orbitrap mass (LTQ and S. of Mass in Mass Spectrom. Scholar). In to the Penning used in the orbitrap of two around which injected ions magnetic are and the of the is a few The is an current of the of ion the and the mass spectrum is as the Fourier transform of this a the has high and it be capable of high mass accuracy. mass accuracy on the of an which is more to achieve than of a magnetic of the mass accuracy of an orbitrap for proteomic have reported Here we that very high mass accuracy is possible on the a background ion produced by in ambient and a number of this ion into the the trap the to the The ions the mass spectrum are then added to this “lock and all are injected into the orbitrap average the mass over the of peptide these average absolute mass in the sub-ppm for at The masses of to the are determined to a few ppm. of was in a 2 and and digested as Mann M. proteomics of high specificity for signaling A. 2003; Scholar). reduce was added to a of 10 in the protein and for at in the The were with for at The and protein mixtures were digested and the peptide mixtures were on as J. Mann M. and for and in Chem. 2003; 75: Scholar) and in for analysis. The which has a and which is therefore an for was from of yeast were in yeast liquid or for 10 of the and yeast determined by were then by for at at two with by and for protein Cell were by in a The yeast was to the was transferred to a and the protein in the was determined by were separated by and to the The was with the were and digested with were into and with For protein were with 10 in for at of was by the with in for at in the were two with with and in a The were with in and for at for protein were transferred to and the remaining were by two with in by with The were and and the used for mass spectrometric analysis. digested peptide mixtures were separated by on-line and analyzed by tandem mass The were on an to an mass spectrometer equipped with a ion and of the in a from with The peptide mixtures were injected the with a of and with a of from in were for and for the yeast The mass spectrometer was in the to between and MS spectra were in the orbitrap with resolution at accumulation to a of in the linear ion The ions to on signal were for in the linear ion trap at a of The fragment ions were in the orbitrap with resolution at For accurate mass measurements the mass was in MS and MS/MS and the ions in the from ambient air A. R. in the ambient air as of background signals in mass Mass Spectrom. 2003; Scholar) were used for internal recalibration in For of the mass into the the mass was at of the of the mass The mass time orbitrap and subsequent spectra was in The time for the and into the of the mass was to be a few at no time in with and mass was in MS/MS the ion at with was used for ions selected for MS/MS were for mass spectrometric no and gas ion gas for Ion was for and time of was applied for were by database an of the protein sequence database or of the for yeast database was with observed and specified an MS tolerance of 10 ppm and an MS/MS tolerance at possible in and specificity for to 2 of was as a and of and were as variable of the high mass the in the yeast database search was a of even into the high fragment mass and with a greater than this were for for peptide mass due to imperfect peaks caused by weak signals we have a that all MS mass measurements of a peptide ion over the LC peak, weighted by signal intensity. For any data all peak and charge of the mass to the peptide is in the measured peptide masses are over the weighted by its signal intensity in The was in and with Thermo Electron data the a in which all peptide ion masses have with the are in and peak for the yeast in the are in the of the orbitrap mass spectrometer have in the A. a of mass Chem. Scholar, M. A. the orbitrap mass to an ion Chem. 2003; 75: Scholar, H. A. M. R. The a mass Mass Spectrom. 2005; Scholar), we the for of the mass accuracy addressed can be in it of The is a capable of MS and MSn spectra at very high but low resolution and mass accuracy. Ions accumulated in the can be transferred into a an quadrupole that and the ions. The to the of the in the of the In the ions are by a low of and to in the of the trap. are injected into the orbitrap high with few Ions are then in the orbitrap by the of the with of the ion Ions to around the and into that the in The of is determined by the of ion from the orbitrap of is by the of injected ion The frequency of this is to the of the mass to charge of the ions and is by a to of the the For a a is produced and the signals of an ion can be into a mass spectrum by Fourier ions are to in the and therefore the the and In the can be with a not with the of the mass of 10 and the of the which has not determined but which is than the of the C-trap. is used as a gas it is used in the of the instrument and it is at capturing and the ions. In the the linear ion trap and fragments it be possible to fragment ions in the it is more and to them in the linear ion trap and in the C-trap. employing the linear ion trap as a the well low mass for fragments to the as The mass of the to in the will be the as in the in is to ion J.C. Senko M.W. A quadrupole ion trap mass Mass Spectrom. Scholar, K. of a ion trap and a ion trap mass spectrometer in Cell Proteomics. 2005; 4: the orbitrap as a high mass in the we injected of a of a a and measured MS and MS/MS spectra with the orbitrap as the were ions for MS and ions for MS/MS in the Analysis of fragments was in the the of the can be with a between acquisition and high to resolution at and MS/MS to a resolution of time for by MS/MS for to of the ions was on from orbitrap accumulation for MS and for and the ion a of a typical mass High and signal to are of the a typical MS/MS spectrum with resolution and a of The that charge of fragment ions is trivial the high resolution and peak in the LTQ, the can to fragments in the or in the orbitrap can be in the the of all ions are as the ion is more in the spectrum, that this into the at the in The between and MS/MS spectra with that on an mass ranges were than and that it was to mass ranges to a MS/MS spectrum J. and M. of high low mass accuracy MS/MS for in Mass Spectrom. Scholar). is by the of ion caused by over the from the to the and from the to the of a spectrum of a peptide ion current of the MS/MS spectrum of a peptide in the and analyzed in the of the ion at Da. that the isotope it to the charge of MS/MS analyzed in the orbitrap in the by 10 The the MS/MS spectrum in the ion in the orbitrap was very as in the observed that of were sufficient to signal to MS/MS spectra. In this experiment, were of the of have even were not for as as the signal is at the of the the as a we of or to filling that are in the of mixtures the is typically by the time in acquisition of the than the ion as was the in this we observed that MS/MS spectra in the orbitrap are less than spectra in the is caused by the high resolution of the orbitrap and its current At ions of the are for and S. of Mass in Mass Spectrom. therefore background ions from which are not to in the spectra. The of MS/MS spectra by in the orbitrap will the acquisition therefore orbitrap MS/MS will be to MS/MS we to the mass accuracy on the mass accuracy was we observed with caused by ambient can be in that mass is much than mass which by a few parts per In mass a mass is to for and to an internal in the spectrum the of For example, was measured in the of a to a sub-ppm mass accuracy Mass for in MALDI Chem. 1999; 71: Scholar), and with a for and internal in mass C.E. calibration on with Fourier transform mass Chem. Scholar). used a ion of which has a composition of and an mass of and is in spectra A. R. in the ambient air as of background signals in mass Mass Spectrom. 2003; Scholar). in a of a few to an a number of background which can all be used as masses for internal calibration during analysis. in mass accuracy of the peptide improved from ppm to ppm by employing as In mass spectrum, we the mass to calibration and all measured by the ppm deviation for all masses as for the the measured mass of the background ion as a of The observed mass is stable less than ppm during time but in the time of spectrum of ambient a of 2 to an in the ambient of these ions can be used as masses during of of the measured mass of a peptide the mass of the background ion the of a mass is well it is not is in to the effort of a mass into the Here we PCM, which is always during the it is not always in or spectra peptide signals to the background ion signals to we of a of the its C-trap. A number of ions used a of is accumulated in the and transferred to the C-trap. In this an signal of is always of the accumulation time used for the mass number of ions not the of the C-trap. of ions and the and no more than a few to the the mass can be added to any For example, ions of can be accumulated in the and a precursor ion can be accumulated and in the LTQ, which is by of all MS/MS ions into the C-trap. of an mass or of masses has into the data and is the mass signal is from the spectra. we the of mass for the of a peptide S.E. B. H. A. Mann M. by in Cell SILAC, as a and to Cell Proteomics. Scholar) yeast was digested with and analyzed by on the The acquisition was as in mass for all spectra. identification of yeast by database mass between calculated and measured peptide masses were in that the of mass is with all or two ppm. the of the few at mass we the mass deviation as a of peptide intensity. that the are mainly caused by low and S. of Mass in Mass Spectrom. Scholar) have reported that signal to is a of achieved mass accuracy in orbitrap mass which is in with on other instruments C.E. Scholar). The data that the mass can reduce the mass error to a few ppm on the of the mass measurement that is the for peptide for improve we of the that several mass measurements are of the precursor as it from the capillary and that these measurements typically are of intensity than the used for precursor the intensity of a yeast peptide as it from the can be in the the precursor was for and its mass determined it was less than of its maximal intensity. mass measurements of the precursor were and it is from that mass accuracy is much at the of the LC peak than it is at its we a to over the LC which the mass measurements weighted by signal intensity. the of these mass accuracy was improved and was a ppm absolute deviation from the calculated values. that all the have a maximal mass error of less than 2 ppm average mass accuracy of 0.48 ppm and a deviation of 0.38 the mass can be applied for MS/MS spectra. however, that the ion of in the during the time it to and fragment the precursor we used this ion for mass scale a and of two peptide spectra in time with the mass spectra were with a of and a resolution of at the mass accuracy to be in the MS/MS with the MS of the and resolution as well as the that a tandem mass spectrum was for all fragments 2 ppm of their calculated provided that the intensity was than with less than were ppm of the calculated in all that the elemental composition of low mass ions can be determined a mass accuracy of a that can be in of tandem mass for example, to peptide sequence M. of in by Peptide Chem. Scholar), sequence B. M. Mann M. Peptide by MALDI tandem mass Proteome Res. Scholar), data sequence of peptide MS/MS data and the of MS/MS Cell Proteomics. 2005; 4: Scholar, protein identification in Fourier mass Cell Proteomics. 2005; 4: Scholar), or in composition B. peptide composition and a employing accurate mass by transform ion cyclotron mass Mass Spectrom. 2004; Scholar). orbitrap MS/MS spectra with the database the achieved mass accuracy is much than can be specified as a search parameter. the not the for mass than or scores to fragment with high mass accuracy J.S. protein identification by sequence mass 1999; Scholar). the the in to the peptide was very large with these high mass accuracy tandem mass in for spectra no peptide sequence was at on the can be in and 2 search with and LC mass and with peptide with and mass Here we a for very high mass accuracy with an mass spectrometer. a background ion of composition into the we for in the over The of this that the mass scale of the that is the of the frequency and of the is at to than per that the remaining mass error mainly on the signal intensity of the peptide For any peaks that are not to the we a mass accuracy to ppm. for weak peaks the mass accuracy is a few ppm. increase the mass we mass measurements over the LC peak weighted by signal intensity. In this several mass measurements to the and the mass is not on a signal to the as is the the precursor mass is the as the which is the for peak for of achieved mass accuracy on signal or signal to is not to the in current proteomic practice, a is The precursor and fragment mass tolerances are to even the mass mass have by recalibration J.S. A. Mann M. Analysis of the proteome by mass Scholar) or by mass as a be to very mass tolerances for well peaks and mass tolerances for weak a be in a all have with a mass In this with signal but large deviation from the calculated masses be from or at a precursor mass measurement be by its as A. A.I. R. to estimate the accuracy of peptide by MS/MS and database Chem. Scholar) can in a The mass PCM, is in other background ions be used as and it is possible to more than mass in the mass of the storage provided by the C-trap. we have used the for a number of mass it can be used for other as For example, the be with several narrow mass ranges of or several MS/MS fragment ions from precursor ions high resolution of the accumulated ions in the In with the the is capable of mass as we achieve the high mass accuracy with the of a mass in the we used the and of a narrow mass into the ICR cell (3Olsen J.V. Ong S.E. Mann M. Trypsin cleaves exclusively C-terminal to arginine and lysine residues.Mol. Cell Proteomics. 2004; 3: 608-614Google Scholar). of the mass is that no time to be on the is and with a high ion at the of its space charge to then mass accuracy is an of than we demonstrate for the is the of the high mass accuracy P. B. for Peptide Characterization by Mass Chem. 1996; Scholar) have that a mass accuracy of ppm peptide to a few and greatly peptide identification. Smith and co-workers added a time and that mass and time be sufficient for peptide identification E.F. Tang K. Smith R.D. Proteome analyses accurate mass and time peptide with capillary LC mass Mass Spectrom. 2003; Scholar). has to mass achieved to have for example, M.E. Smith R.D. A proteomic of the Proteome an accurate mass and time 2005; 5: Scholar). with the accuracy reported we not that the mass is sufficient to in typical proteomic the introduced by and peptide for as of the number of candidate peptide will be very and even low accuracy tandem mass spectra can then the candidate peptide is this mass accuracy will be in the of which a problem of the caused of S.E. Mann M. and in by 2004; Scholar). In we have that a compact mass the is capable of very high mass accuracy a mass High mass accuracy is in the MS and MS/MS and or in combination with strategies J.V. Mann M. peptide identification in proteomics by two of mass spectrometric A. 2004; Scholar) to the problem of false positive peptide identification in proteomics and to much more than in the for and Cell as well as at the for with