Th R was originally developed to assess the contribution of the targeted precursor in a fragmentation isolation window using a metric called “precursor ion purity”. See associated paper (Lawson et al. 2017).
A number of updates have been made since the original paper and the full functionality of msPurity now includes the following:
What we call “Precursor ion purity” is a measure of the contribution of a selected precursor peak in an isolation window used for fragmentation. The simple calculation involves dividing the intensity of the selected precursor peak by the total intensity of the isolation window. When assessing MS/MS spectra this calculation is done before and after the MS/MS scan of interest and the purity is interpolated at the time of the MS/MS acquisition. The calculation is similar to the “Precursor Ion Fraction”" (PIF) metric described by (Michalski, Cox, and Mann 2011) for proteomics with the exception that purity here is interpolated at the recorded point of MS/MS acquisition using bordering full-scan spectra. Additionally, low abundance ions that are remove that are thought to have limited contribution to the resulting MS/MS spectra and the isolation efficiency of the mass spectrometer can be used to normalise the contributing ions to metric.
There are 3 main classes used in msPurity
Given a vector of LC-MS/MS or DIMS/MS mzML file paths the precursor ion purity of each MS/MS scan can be calculated and stored in the purityA S4 class object where a dataframe of the purity results can be accessed using the appropriate slot (pa@puritydf
).
The calculation involves dividing the intensity of the selected precursor peak by the total intensity of the isolation window and is performed before and after the MS/MS scan of interest and interpolated at the recorded time of the MS/MS acquisition. See below
Additionally, isotopic peaks can estimated and omitted from the calculation, low abundance peaks are removed that are thought to have limited contribution to the resulting MS/MS spectra and the isolation efficiency of the mass spectrometer can be used to normalise the intensities used for the calculation.
The purity dataframe (pa@puritydf
) consists of the following columns:
The remaining slots for purityA class include
library(msPurity)
mzMLpths <- list.files(system.file("extdata", "lcms", "mzML", package="msPurityData"), full.names = TRUE, pattern = "MSMS")
Note that if there are any mzML files that do not have MS/MS scans - then an ID is save of the file but no assessments will be made.
pa <- purityA(mzMLpths)
print(pa@puritydf[1:3,])
## pid fileid seqNum acquisitionNum precursorIntensity precursorMZ
## 1 1 1 7 7 2338044 391.2838
## 2 2 1 8 8 1415940 149.0232
## 3 3 1 9 9 1319700 135.1015
## precursorRT precursorScanNum id filename retentionTime
## 1 2.707016 6 7 LCMSMS_1.mzML 2.977597
## 2 2.707016 6 8 LCMSMS_1.mzML 3.070549
## 3 2.707016 6 9 LCMSMS_1.mzML 3.163231
## precursorNearest aMz aPurity apkNm iMz iPurity ipkNm inPkNm
## 1 6 391.2838 1.0000000 1 391.2838 1.0000000 1 1
## 2 6 149.0233 0.8535700 2 149.0233 0.8535700 2 2
## 3 6 135.1015 0.7616688 4 135.1015 0.7616688 4 4
## inPurity
## 1 1.0000000
## 2 0.8475240
## 3 0.7558731
We define here “isolation efficiency”" as the effect of the position of an ion within an isolation window on its relative intensity in corresponding fragmentation spectra. When the isolation efficiency of an instrument is known, the peak intensities within an isolation window can be normalised for the precursor purity calculation. In the example in beloq, an R-Cosine isolation efficiency curve is used, the red peak (the targeted precursor ion peak) would not change following normalisation - as the contribution is at 1 (i.e. 100%) - however the the black peak (a contaminating ion) would be normalised by approximately 0.1 (i.e. 10%) and the normalised intensity would be calculated as 1000 (i.e. original intensity of 10000 x 0.1)
The isolation efficiency can be estimated by looking at a single precursor with a sliding window - see below for an example deomonstrating a sliding window around a target m/z of 200.
A sliding window experiment has been performed to assess Thermo Fisher Q-Exactive Mass spectrometer using 0.5 Da windows and can be set within msPurity by using msPurity::iwNormQE.5() as the input to the iwNormFunc argument. See below:
Other available options are to use gaussian isolation window msPurity::iwNormGauss(minOff=-0.5, maxOff = 0.5) or a R-Cosine window msPurity::iwNormRCosine(minOff=-0.5, maxOff=0.5). Where the minOff and maxOff can be changed depending on the isolation window.
A user can also create their own normalisation function. The only requirement of the function is that given a value between the minOff and maxOff a normalisation value between 0-1 is returned.
Se below for example of using one of the default provided normalisation functions.
msmsPths <- list.files(system.file("extdata", "lcms", "mzML", package="msPurityData"), full.names = TRUE, pattern = "MSMS")
pa_norm <- purityA(msmsPths[1], iwNorm=TRUE, iwNormFun=iwNormGauss(sdlim=3, minOff=-0.5, maxOff=0.5))
If the isolation efficiency of the instrument is not known, by default iwNorm is set to FALSE and no normalisation will occur.
First an xcmsSet object of the same files is required
suppressPackageStartupMessages(library(xcms))
xset <- xcms::xcmsSet(mzMLpths)
xset <- xcms::group(xset)
Then the MS/MS spectra can be assigned to an XCMS grouped feature using the frag4feature
function.
pa <- frag4feature(pa, xset)
The slot grped_df
is a dataframe of the grouped XCMS features linked to a reference to any associated MS/MS scans in the region of the full width of the XCMS feature in each file. The dataframe contains the following columns.
print(head(pa@grped_df[1:3]))
## grpid mz mzmin
## 1 8 112.0509 112.0506
## 2 8 112.0508 112.0507
## 3 12 116.0706 116.0109
## 4 12 116.0706 116.0109
## 5 12 116.0706 116.0109
## 6 12 116.0706 116.0109
The slot grped_MS2
is a list of the associated fragmentation spectra for the grouped features.
print(pa@grped_ms2[[1]]) # fragmentation associated with the first XCMS grouped feature (i.e. xset@groups[1,])
## [[1]]
## [,1] [,2]
## [1,] 112.0509 565117.250
## [2,] 126.5377 2499.315
##
## [[2]]
## [,1] [,2]
## [1,] 112.0509 440629.7
Flag and filter features based on signal-to-noise ratio, relative abundance, intensity threshold and precursor ion purity of the precursor.
pa <- filterFragSpectra(pa)
Average and filter fragmentation spectra for each XCMS feature within and across MS data files (ignoring intra and inter relationships).
pa <- averageAllFragSpectra(pa)
Average and filter fragmentation spectra for each XCMS feature within a MS data file.
pa <- averageIntraFragSpectra(pa)
Average and filter fragmentation spectra for each XCMS feature across MS data files. This can only be run after averageIntraFragSpectra has been used.
pa <- averageInterFragSpectra(pa)
Create an MSP file for all the fragmentation spectra that has been linked to an XCMS feature via frag4feature. Can export all the associated scans individually or the averaged fragmentation spectra can be exported.
Additional metadata can be included in a dataframe (each column will be added to metadata of the MSP spectra). The dataframe must contain the column “grpid” corresponding to the XCMS grouped feature.
td <- tempdir()
createMSP(pa, msp_file_pth = file.path(td, 'out.msp'))
A database can be made of the LC-MS/MS dataset - this can then be udpated with the spectral matching data (from spectralMatching function). The full schema of the database is found here. This replaces the old schema used by the deprecated function spectral_matching.
q_dbPth <- createDatabase(pa, xset, outDir = td, dbName = 'test-mspurity-vignette.sqlite')
A query SQLite database can be matched against a library SQLite database with the spectralMatching function. The library spectral-database in most cases should contain the “known” spectra from either public or user generated resources. The library SQLite database by default contains data from MoNA including Massbank, HMDB, LipidBlast and GNPS. A larger database can be downloaded from here.
result <- spectralMatching(q_dbPth, q_xcmsGroups = c(12, 27), cores=1, l_accessions=c('CCMSLIB00000577898','CE000616'))
## Running msPurity spectral matching function for LC-MS(/MS) data
## Filter query dataset
## Filter library dataset
## aligning and matching
## Summarising LC feature annotations
NOTE ON TERMINOLOGY: The term ‘anticipated purity’ and ‘predicted purity’ are used interchangeably
A processed xcmsSet object is required to determine the anticipated (predicted) precursor purity score from an LC-MS dataset. The offsets chosen in the parameters should reflect what settings would be used in a hypothetical fragmentation experiment.
The slot predictions
provides the anticipated (predicted) purity scores for each feature. The dataframe contains the following columns:
XCMS run on an LC-MS dataset
msPths <- list.files(system.file("extdata", "lcms", "mzML", package="msPurityData"), full.names = TRUE, pattern = "LCMS_")
#Run xcms
#xset <- xcmsSet(msPths)
#xset <- group(xset)
# Or load an XCMS xcmsSet object saved earlier
xset <- readRDS(system.file("extdata", "tests", "xcms", "ms_only_xset.rds", package="msPurity"))
# Make sure the file paths are correct
xset@filepaths[1] <- msPths[basename(msPths)=="LCMS_1.mzML"]
xset@filepaths[2] <- msPths[basename(msPths)=="LCMS_2.mzML"]
Perform purity calculations
px <- purityX(xset, cores = 1, xgroups = c(1, 2), ilim=0)
The anticipated/predicted purity for a DIMS experiment can be performed on any DIMS dataset consisting of multiple MS1 scans of the same mass range, i.e. it has not been developed to be used with any SIM stitching approach.
A number of simple data processing steps are performed on the mzML files to provide a DIMS peak list (features) to perform the purity predictions on.
These data processing steps consist of:
The averaged peaks before and after filtering are stored in the avPeaks
slot of purityPD S4 object.
Get file dataframe: The purityD constructor requires a dataframe consisting of the following columns:
datapth <- system.file("extdata", "dims", "mzML", package="msPurityData")
inDF <- Getfiles(datapth, pattern=".mzML", check = FALSE)
ppDIMS <- purityD(inDF, mzML=TRUE)
Average spectra: The default averaging will use a Hierarchal clustering approach. Noise filtering is also performed here.
ppDIMS <- averageSpectra(ppDIMS, snMeth = "median", snthr = 5)
Filter by RSD and Intensity
ppDIMS <- filterp(ppDIMS, thr=5000, rsd = 10)
Subtract blank
ppDIMS <- subtract(ppDIMS)
Predict purity
ppDIMS <- dimsPredictPurity(ppDIMS)
print(head(ppDIMS@avPeaks$processed$B02_Daph_TEST_pos))
## peakID mz i snr rsd inorm count total
## 5 5 173.0806 11272447.0 216.506319 9.006126 0.0108585920 5 4
## 7 7 179.1177 606983.2 11.425825 6.019861 0.0005729283 5 4
## 10 10 217.1067 17770220.0 343.292914 8.602331 0.0171178067 5 4
## 15 15 235.1173 4950841.5 95.991762 6.302825 0.0047694791 5 4
## 16 16 236.1206 486912.0 9.270517 8.811437 0.0004638254 5 4
## 17 17 239.1485 2533134.5 48.892062 5.781277 0.0024401334 5 4
## medianPurity meanPurity sdPurity cvPurity sdePurity medianPeakNum
## 5 1.0000000 1.0000000 0.00000000 0.000000 0.000000000 1
## 7 1.0000000 1.0000000 0.00000000 0.000000 0.000000000 1
## 10 0.7797864 0.7808917 0.01261501 1.615462 0.005641605 2
## 15 1.0000000 1.0000000 0.00000000 0.000000 0.000000000 1
## 16 0.8818313 0.8755873 0.01056807 1.206969 0.004726184 2
## 17 0.8123950 0.8229505 0.04384595 5.327896 0.019608505 2
The data processing steps carried out through purityPD can be bypassed if the peaks (m/z values) of interest are already known. The function dimsPredictPuritySingle()
can be used to predict the purity of a list of m/z values in a chosen mzML file.
mzpth <- system.file("extdata", "dims", "mzML", "B02_Daph_TEST_pos.mzML", package="msPurityData")
predicted <- dimsPredictPuritySingle(filepth = mzpth, mztargets = c(111.0436, 113.1069))
print(predicted)
Lawson, Thomas Nigel, Ralf J. M. Weber, Martin R. Jones, Andrew J. Chetwynd, Giovanny Alejandro Rodriguez Blanco, Riccardo Di Guida, Mark R. Viant, and Warwick B Dunn. 2017. “msPurity: Automated Evaluation of Precursor Ion Purity for Mass Spectrometry Based Fragmentation in Metabolomics.” Analytical Chemistry, acs.analchem.6b04358. https://doi.org/10.1021/acs.analchem.6b04358.
Michalski, Annette, Juergen Cox, and Matthias Mann. 2011. “More than 100,000 detectable peptide species elute in single shotgun proteomics runs but the majority is inaccessible to data-dependent LC-MS/MS.” Journal of Proteome Research 10 (4):1785–93. https://doi.org/10.1021/pr101060v.