Patent Description:
Mass spectrometry is a long established technique for identification and quantitation of often complex mixtures of large organic molecules. In recent years, techniques have been developed that allow analysis of a wide range of both biological and non-biological materials, with application across the fields of law enforcement (e.g. identification of drugs and explosives materials), environmental, scientific research, and biology (e.g. in proteomics, the study of simple and complex mixtures of proteins, with applications in drug discovery, disease identification and so forth).

Proteins, comprising large numbers of amino acids, are typically of significant molecular weight. Thus accurate identification and quantitation of the protein by direct mass spectrometric measurement is challenging. It is thus well known to carry out fragmentation of the precursor sample material. A variety of fragmentation techniques are known, which may result in the generation of different fragment ions from the precursor ions. Moreover, the fragmentation mechanism may be affected by different applied fragmentation energies.

Analysis of samples can broadly be separated into data independent analysis/acquisition (DIA) and data dependent analysis/acquisition (DDA) techniques. DIA seeks to determine what is present in a sample of potentially unknown identity. To determine the molecular structure of sample molecules, a mass spectrometer is first used to mass analyse all sample ions (precursor ions) within a selected window of mass to charge ratio (m/z). Such a scan is often denoted as an MS1 scan. The selected sample ions are then fragmented and the resulting fragments are subsequently mass analysed across the selected m/z range. The scan of the fragmented ions is often denoted as an MS2 scan.

DDA by contrast, seeks to confirm that one or more species is/are present in a given sample. Methods of DDA identify a fixed number of precursor ion species, and select and analyse those via mass spectrometry. The determination of which precursor ion species are of interest in DDA may be based upon intensity ranking (for example, the top ten most abundant species as observed by peaks in a MS1 spectrum"), or by defining an "inclusion list" of precursor mass spectral peaks (for example by user selection), from which MS2 spectra are always acquired regardless of the intensity ranking of the peak in the MS1 mass spectrum. Still otherwise, an "exclusion list" of peaks in MS1 can be defined, for example by a user, based e.g. on prior knowledge of the expected sample contents.

DIA avoids the decisions necessary in DDA, by simply dividing the mass range of interest (typically user defined) into segments and obtaining MS2 spectra for each segment. With DIA, the acquisition of an MS1 precursor spectrum becomes more or less optional, since the parameters of the selection window for the sample ions carries information about the range of possible sample ions within that window.

Early DIA techniques were disclosed in patent applications by Micromass UK Ltd and Waters Technologies Corporation, in their so-called MSE arrangements. The DIA techniques resulted from application of known triple quadrupole methods to quadrupole-TOF arrangements.

In <CIT>, a technique is disclosed in which MS1 and MS2 are alternatively acquired by repeatedly switching the energy of the fragmentation cell. The technique relies upon separation of the sample molecules through different elution times in a chromatography environment. At the end of an experimental run, precursor and fragment ions are recognized by comparing the mass spectra in the two different fragmentation modes. Fragment ions are matched to particular precursor ions on the basis of the closeness of fit of their elution times, so that precursor ions can then be identified.

<CIT> discloses a development to the DIA technique in the `<NUM> patent described above. Here, the energy applied to the fragmentation cell is again repeatedly switched so as to obtain both MS1 and MS2. However here MS1 and MS2 are obtained from both a first and a second sample separately.

The mass spectra are then compared and further analysis is carried out where precursor ions in MS1 from each sample, or fragment ions in MS2 from each sample, are expressed differently.

Finally <CIT> again employs switching between energy levels in the fragmentation chamber so as to generate MS1 and MS2 in alternating manner. Comparison of the chromatographic peak shape of the precursor and fragment peaks is carried out to identify an association between precursor and fragment (product) ions.

An alternative approach to DIA, known as "SWATH", has been proposed in various patents to DH Technologies Development Pte.

In <CIT>, a DIA data set is acquired such that the data may subsequently be analysed for a target substance. This contrasts with the idea of setting a target and then acquiring data only for that purpose. The method employs LC-MS and uses wide windows of precursor ions (e.g. ><NUM>, ><NUM>, ><NUM> amu) for MS2, allowing the whole precursor space to be covered.

Again the '<NUM> patent stresses the importance of retaining the fidelity of the chromatographic peaks in the MS2 spectrum, by appropriate setting of the windows. An MS1 spectrum is indicated to be optional.

As an example, the '<NUM> patent describes a method - akin to single reaction monitoring (SRM) - for evaluation of the MS2 data of a precursor mass window as a function of retention time, and for subsequent comparison with a reference spectrum library.

<CIT> employs isolation windows for the precursor ions, of variable width, the width being dependent upon the precursor mass. The method trades off analysis speed (for a wide window) and sensitivity/specificity (for a narrow window).

<CIT> addresses drawbacks with the methods disclosed in <CIT> by scoring extracted ion chromatogram (XIC) peak candidates based on various criteria, in a comparison between the XIC fragment peaks with the MS1 information, such as mass accuracy, charge state, isotopic state, known neutral losses and so forth.

A common aspect of the approach in the MSE and SWATH techniques described above is that they seek to optimize measurements for good MS2 time resolution. To obtain sufficient data points across the LC peak for good quantitation, either a relatively wide precursor isolation window (24Da) - as suggested in the MSE patents discussed above - or a variable width precursor isolation window (the preferred approach for the SWATH patents discussed above) needs to be employed.

The consequence is that the traditional database search - in which sample fragment spectra are compared against fragment spectra of known species in a library, as is the case with DDA - may not be well suited for DIA data analysis. In the case of the SWATH technique, a large spectral library must first be created (for the same or similar sample types) for targeted extraction of MS2 chromatograms from convoluted spectra, which is an expensive and time consuming task.

In "<NPL>) a method of DIA analysis using a tandem mass spectrometer is disclosed. In particular, an Orbitrap mass spectrometer is used to perform MS1 scans of precursor ions, whilst a linear ion trap is used to perform MS2 analysis of the fragmented ions using a mass window of <NUM> amu for each MS2 scan. By using a narrow mass window, the resulting data can be directly used for database searching, realizing the integration of DDA and DIA methodologies.

"<NPL> discloses a method of DIA mass spectrometry.

For DIA methodologies performed on narrow chromatographic peaks of the order of several seconds, one ideally needs to sample the chromatographic peak at least seven or better still at least ten times over the full m/z range. This requirement constantly forces shorter and shorter DIA cycle times, currently <NUM>-<NUM> seconds is considered the upper limit of allowed cycle time for applications in proteomics and metabolomics. At the same time, the requirement for deeper coverage of different proteomes/metabolomes leads to bigger and bigger spectral libraries being required for quantitation of the DIA data.

The present inventors have realised that one problem with existing DIA methodologies is that large spectral libraries of fragment spectra are required for quantitation of fragment spectra in the MS2 domain. The present inventors have realised that it would be desirable to move to a library free approach for DIA analysis of samples. In order to achieve such library free analysis, the present inventors propose a method and apparatus that enables significantly higher specificity and speed of DIA.

For example, a method of DIA analysis using a mass window of <NUM> amu for each MS2 scan is discussed above. This relatively narrow mass window is similar to the targeted mass windows used in a known DDA approach. By using relatively narrow mass windows for each of the MS2 scans, the resulting MS2 spectra may be analysed using DDA type databases, rather than requiring full DIA-specific spectral libraries.

The present inventors have identified that one problem with using such a narrow mass window for each of the MS2 scans, is that the number of scans required to build up a full range of MS2 scans for the mass range of interest increases. As a result, the time taken to perform a complete DIA analysis can become overly long, for example much longer than the duration of a chromatographic peak. If the DIA analysis is not completed within the duration of the chromatographic peak, the analysis may not provide meaningful data, as some parts of the analysis will not measure the sample peak.

Furthermore, another problem identified by the inventors with this approach, is that the relatively narrow mass windows for each MS2 scan result in relatively few, if any, fragmenting ions reaching the detector at a given time. Thus, reducing the mass selection window for each MS2 scan results in a reduction in the mass accuracy and/or the sensitivity of the MS2 mass analyser. This problem is exacerbated when attempting to perform a large number of MS2 scans at a sufficient frequency to fit all MS2 scans within the duration of a chromatographic peak.

The present invention seeks to address the shortcomings of existing DIA approaches. In accordance with a first aspect of the present invention, there is provided a method of data independent analysis (DIA) in accordance with claim <NUM>. The invention also extends to a mass spectrometer in accordance with claim <NUM>.

In order to acquire data suitable for identification/quantitation of precursor ions using a DDA type database, the present invention acquires MS1 and MS2 spectra utilising high resolution, high mass accuracy mass analysers. In particular, in the MS2 domain, the present invention acquires MS2 spectra of narrow mass segments of less than <NUM> amu. In this way, the MS2 spectra can be analysed with DDA-type databases. In particular, it is important that the MS2 spectra are acquired using high mass accuracy, high resolution mass analysers in order to identify fragments with sufficient accuracy for the DDA-type databases to be applicable.

Advantageously, by utilising a Time of Flight (TOF) mass analyser in tandem with a FTMS mass analyser, high mass accuracy scans may be performed in both the MS1 and MS2 domains. Furthermore, the MS2 scans utilise a TOF mass analyser which is preferably operated at a frequency of at least <NUM> in order to perform the plurality MS2 scans of the precursor mass segments of less than <NUM> amu. By performing the plurality of MS2 scans at such a frequency, MS2 spectra corresponding to narrow windows of precursor ions may be acquired across the full mass range of interest within a cycle time that allows the DIA methodology to fully sample a chromatographic peak.

Importantly, MS1 data may be acquired across the full mass range of interest in tandem with the acquiring of the MS2 data. By utilising a FTMS mass analyser, high resolution high mass accuracy MS1 data may also be acquired to complement the MS2 data. Furthermore, by acquiring the MS1 data in tandem with the MS2 data, the total cycle time may be reduced compared to performing MS1 scans serially with the MS2 scans.

According to the invention, the fragmented ions are accumulated prior to injection into the time of flight mass analyser. By accumulating fragmented ions for a predetermined time (duration) prior to mass analysis in the MS2 domain, the number of fragmented ions in each packet of ions is increased. Methods and apparatus for accumulation of ions are described below. This may lead, in preferred embodiments, to all fragmented ions being utilised for MS2 scans, thereby increasing the duty cycle. As a time of flight mass analyser is used to mass analyse each packet of fragmented ions, by increasing the number of ions in each packet, the intensity of the signal detected at a detector of the time of flight mass analyser is increased.

Preferably, the time of flight mass analyser is operated at a frequency of at least <NUM> or at least: <NUM>, <NUM>, <NUM> or <NUM>. By providing a minimum operating frequency for the TOF mass analyser, the total cycle time of the DIA methodology may be reduced relative to the duration of the chromatographic peak, and thus ensuring that the sample ions are suitably sampled. Preferably, the TOF mass analyser is operated at a frequency no greater than <NUM>, or more preferably <NUM>, <NUM> or <NUM> in order to provide sufficient time for the accumulation fragmented ions prior to the injection into the TOF analyser. Advantageously, by accumulating fragmented ions and mass analysing the fragmented ions as a packet, the resolution and mass accuracy of the resulting MS2 scans may be increased, whilst still achieving a suitable frequency of operation which allows for the analysis of a relatively wide mass range (e.g. <NUM>-<NUM>/z) over the duration of a chromatographic peak.

Preferably, the present invention utilises an orbital trapping mass analyser to perform relatively high resolution MS1 scans of the precursor ions. Thus, data in the MS1 domain may also be captured with high resolution and high mass accuracy. Other mass analysers of high resolution could be utilised as the first mass analyser to perform the MS1 scans. For example, an ion cyclotron resonance (ICR) mass analyser or a time of flight mass analyser (especially a multi-reflection time of flight mass analyser).

Preferably, the FTMS mass analyser performs MS1 scans at a mass resolution of at least <NUM>,<NUM>, or more preferably at least: <NUM>,<NUM>, <NUM>,<NUM>, <NUM>,<NUM> or <NUM>,<NUM> (resolution at <NUM>/z). Where other types of mass analyser are used for the MS1 scans of the precursor ions, they also preferably perform the MS1 scans at a mass resolution of at least <NUM>,<NUM>, or more preferably at least: <NUM>,<NUM>, <NUM>,<NUM>, <NUM>,<NUM> or <NUM>,<NUM> (resolution at <NUM>/z). By performing MS1 scans at such a mass resolution, the MS1 data may be more suitable for analysis using a DDA-type library thus resulting in increased accuracy of precursor quantitation/identification.

Preferably, the present invention utilises a multiple reflection time of flight mass analyser (mr-TOF) to perform the plurality of MS2 scans. By utilising a mr-TOF, the flight time of the packets of fragmented ions may be increased due to the multiple reflections included in the flight path of the ions packets through the mr-TOF. Utilising a relatively long flight path, for example in excess of <NUM>, or <NUM>, or preferably <NUM>, or more preferably <NUM> is advantageous, as it increases the time resolution of each packet arriving at the detector in the mr-TOF and may reduce adverse space-charge effects. Examples of mr-TOF mass analysers include orbital-type mr-TOF analysers as described in <CIT> or tilted-mirror type mr-TOF analysers as described in <CIT>. Thus the resolution of MS2 scans using an mr-TOF may be increased without requiring an increase in measurement time for each scan. Accordingly, a plurality of narrow mass window (i.e. less than <NUM> amu) MS2 scans may be performed within the duration of a chromatographic peak in accordance with the methodology of the present invention. Preferably, the mass range of each segment of precursor ions scanned in the MS2 domain is not greater than <NUM> amu, or more preferably not greater than: <NUM> amu or <NUM> amu. By reducing the mass range of each segment of precursor ions fragmented for MS2 analysis, the resulting MS2 spectrum has a reduced number of possible precursor ions from which it was formed. Accordingly, the complexity of the resulting MS2 spectra may be reduced, thereby improving the subsequent analysis of the MS2 spectra for quantitation and/or identification of precursor ions.

Preferably, the mass resolution of the TOF mass analyser is at least <NUM>,<NUM> for each of the MS2 scans (resolution at <NUM>/z). More preferably, the resolution of the TOF analyser is at least <NUM>,<NUM> or <NUM>,<NUM>. By providing MS2 scans at such a resolution, the mass accuracy of the MS2 spectra may be matched to the corresponding high resolution, high mass accuracy MS1 scans and/or may be matched to DDA-type databases for quantitation and/or identification of the sample.

According to the invention, at least X% of the MS2 scans contain more than Y ion counts, wherein X= <NUM>, or <NUM>, or <NUM>, or <NUM>, and Y= <NUM>, or <NUM>, or <NUM>, or <NUM>, or <NUM>. By ensuring that at least a specified percentage of the MS2 scans have a minimum ion count, the dynamic range of the MS2 scans may be increased. Accordingly, the mass accuracy of the resulting MS2 data is increased.

Preferably, the DIA methodology is repeated a number of times over the duration of a chromatographic peak. Accordingly, the cycle time of the DIA measurement may be adapted to be performed a plurality of times over the duration of a chromatographic peak. By performing the DIA methodology a number of times over the duration of the chromatographic peak, the peak may be sampled a number of times, allowing a complete picture of the peak to be established. Preferably, the DIA methodology is performed at least: <NUM>, <NUM>, <NUM>, <NUM>, <NUM> or more preferably <NUM> times over the duration of a chromatographic peak.

Preferably, the performing of the MS1 scan of the precursor ions across the mass range of interest further comprises separating the precursor ions in the mass range of interest into a plurality of mass sub-ranges, and for each mass sub-range of precursor ions mass analysing the sub-range of precursor ions using the Fourier Transform mass analyser. As such, the MS1 scan of the precursor ions in the mass range of interest is split into a set (plurality) of MS1 scans of a plurality of mass sub-ranges of the precursor ions, wherein the combination of the plurality of mass sub-ranges make up the mass range of interest. By separating the MS1 scan into a set of MS1 scans, space charge effects associated with the relatively wide precursor mass range may be reduced. Preferably, the mass range of the precursor ions in each mass sub-range is no greater than <NUM> amu, or more preferably <NUM> amu, or more preferably <NUM> amu. By reducing the mass range of each mass sub-range, space charge effects may be further reduced.

Preferably, the mass range of interest has a mass range of at least <NUM> amu, more preferably at least <NUM> amu, or more preferably at least <NUM> amu. For example, the mass range of interest may be <NUM>/z to <NUM>/z. By varying the width of the mass range of interest, the time for performing the DIA analysis may be adapted in order to correspond to the duration of a chromatographic peak. The precursor mass range of interest may also be chosen based on a desired mass range of precursor ions to be analysed.

In a preferred embodiment, the invention comprises: separating the precursor ions into a plurality of precursor mass sub-ranges across the mass range of interest;
wherein for each precursor mass sub-range:.

Preferably, performing an MS2 scan of the set of MS2 scans includes combining fragmented ions from a plurality of precursor mass segments such that the combined fragmented ions are mass analysed. Preferably, a plurality of precursor mass segments are fragmented together and subsequently mass analysed together. Preferably, the data resulting in this way from the set of MS2 scans is deconvoluted to obtain MS2 spectra for each of the precursor mass segments. In another preferred embodiment, a plurality of precursor mass segments are fragmented separately, e.g. separately in time (sequentially), and subsequently mass analysed together (optionally in wherein the set of MS2 scans is deconvoluted to obtain MS2 spectra for each of the precursor mass segments). By performing MS2 scans of a plurality of precursor mass segments at the same time, the time taken to obtain the MS2 spectra may be reduced. Additionally, the method allows one or more of the precursor mass segments to be mass analysed as part of more than one combination. Thus, the mass accuracy of the resulting MS2 mass spectra may be improved as a result of multiple MS2 scans of precursor mass segments.

The invention may be put into practice in a number of ways and specific embodiments will now be described by way of example only and with reference to the Figures in which:.

Herein the term mass may be used to refer to the mass-to-charge ratio, m/z. The resolution of a mass analyser is to be understood to refer to the resolution of the mass analyser as determined at a mass to charge ratio of <NUM> unless otherwise stated.

<FIG> shows a schematic arrangement of a mass spectrometer <NUM> suitable for carrying out methods in accordance with embodiments of the present invention.

In <FIG>, a sample to be analysed is supplied (for example from an autosampler) to a chromatographic apparatus such as a liquid chromatography (LC) column (not shown in <FIG>). One such example of an LC column is the Thermo Fisher Scientific, Inc ProSwift monolithic column which offers high performance liquid chromatography (HPLC) through the forcing of the sample carried in a mobile phase under high pressure through a stationary phase of irregularly or spherically shaped particles constituting the stationary phase. In the HPLC column, sample molecules elute at different rates according to their degree of interaction with the stationary phase.

A chromatograph may be produced by measuring over time the quantity of sample molecules which elute from the HPLC column using a detector (for example a mass spectrometer). Sample molecules which elute from the HPLC column will be detected as a peak above a baseline measurement on the chromatograph. Where different sample molecules have different elution rates, a plurality of peaks on the chromatograph may be detected. Preferably, individual sample peaks are separated in time from other peaks in the chromatogram such that different sample molecules do not interfere with each other.

On a chromatograph, a presence of a chromatographic peak corresponds to a time period over which the sample molecules are present at the detector. As such, a width of a chromatographic peak is equivalent to a time period over which the sample molecules are present at a detector. Preferably, a chromatographic peak has a Gaussian shaped profile, or can be assumed to have a Gaussian shaped profile. Accordingly, a width of the chromatographic peak can be determined based on a number of standard deviations calculated from the peak. For example, a peak width may be calculated based on <NUM> standard deviations of a chromatographic peak. Alternatively, a peak width may be calculated based on the width at half the maximum height of the peak. Other methods for determining the peak width known in the art may also be suitable.

The sample molecules thus separated via liquid chromatography are then ionized using an electrospray ionization source (ESI source) <NUM> which is at atmospheric pressure.

Sample ions then enter a vacuum chamber of the mass spectrometer <NUM> and are directed by a capillary <NUM> into an RF-only S lens <NUM>. The ions are focused by the S lens <NUM> into an injection flatapole <NUM> which injects the ions into a bent flatapole <NUM> with an axial field. The bent flatapole <NUM> guides (charged) ions along a curved path through it whilst unwanted neutral molecules such as entrained solvent molecules are not guided along the curved path and are lost.

An ion gate (TK lens) <NUM> is located at the distal end of the bent flatapole <NUM> and controls the passage of the ions from the bent flatapole <NUM> into a downstream mass selector in the form of a quadrupole mass filter <NUM>. The quadrupole mass filter <NUM> is typically but not necessarily segmented and serves as a band pass filter, allowing passage of a selected mass number or limited mass range whilst excluding ions of other mass to charge ratios (m/z). The mass filter can also be operated in an RF-only mode in which it is not mass selective, i.e. it transmits substantially all m/z ions. For example, the quadrupole mass filter <NUM> may be controlled by the controller <NUM> to select a range of mass to charge ratios to pass of the precursor ions which are allowed to mass, whilst the other ions in the precursor ion stream are filtered. Alternatively, the S lens <NUM> may be operated as an ion gate and the ion gate (TK lens) <NUM> may be a static lens.

Although a quadrupole mass filter is shown in <FIG>, the skilled person will appreciate that other types of mass selection devices may also be suitable for selecting precursor ions within the mass range of interest. For example, an ion separator as described in <CIT>, an ion trap as described in <CIT>, an ion mobility separator as described in <CIT>, an ion gate mass selection device as described in <CIT>, or a charged particle trap as described in <CIT>. The skilled person will appreciate that other methods selecting precursor ions according to ion mobility, differential mobility and/or transverse modulation may also be suitable.

The isolation of a plurality of ions of different masses or mass ranges may also be performed using the method known as synchronous precursor scanning (SPS) in an ion trap. Furthermore, in some embodiments, more than one ion selection or mass selection device may be provided. For example, a further mass selection device may be provided downstream of the fragmentation chamber <NUM>. In this way, MS<NUM> or MSn scans can be performed if desired (typically using the TOF mass analyser for mass analysis).

Ions then pass through a quadrupole exit lens/split lens arrangement <NUM> and into a first transfer multipole <NUM>. The first transfer multipole <NUM> guides the mass filtered ions from the quadrupole mass filter <NUM> into a curved linear ion trap (C-trap) <NUM>. The C-trap (first ion trap) <NUM> has longitudinally extending, curved electrodes which are supplied with RF voltages and end caps that to which DC voltages are supplied. The result is a potential well that extends along the curved longitudinal axis of the C-trap <NUM>. In a first mode of operation, the DC end cap voltages are set on the C-trap so that ions arriving from the first transfer multipole <NUM> are captured in the potential well of the C-trap <NUM>, where they are cooled. The injection time (IT) of the ions into the C-trap determines the number of ions (ion population) that is subsequently ejected from the C-trap into the mass analyser.

Cooled ions reside in a cloud towards the bottom of the potential well and are then ejected orthogonally from the C-trap towards the first mass analyser <NUM>. As shown in <FIG>, the first mass analyser is an orbital trapping mass analyser <NUM>, for example the Orbitrap® mass analyser sold by Thermo Fisher Scientific, Inc. The orbital trapping mass analyser <NUM> has an off centre injection aperture and the ions are injected into the orbital trapping mass analyser <NUM> as coherent packets, through the off centre injection aperture. Ions are then trapped within the orbital trapping mass analyser by a hyperlogarithmic electric field, and undergo back and forth motion in a longitudinal direction whilst orbiting around the inner electrode.

The axial (z) component of the movement of the ion packets in the orbital trapping mass analyser is (more or less) defined as simple harmonic motion, with the angular frequency in the z direction being related to the square root of the mass to charge ratio of a given ion species. Thus, over time, ions separate in accordance with their mass to charge ratio.

Ions in the orbital trapping mass analyser are detected by use of an image detector (not shown) which produces a "transient" in the time domain containing information on all of the ion species as they pass the image detector. The transient is then subjected to a Fast Fourier Transform (FFT) resulting in a series of peaks in the frequency domain. From these peaks, a mass spectrum, representing abundance/ion intensity versus m/z, can be produced.

In the configuration described above, the sample ions (more specifically, a mass range segment of the sample ions within a mass range of interest, selected by the quadrupole mass filter) are analysed by the orbital trapping mass analyser without fragmentation. The resulting mass spectrum is denoted MS1.

Although an orbital trapping mass analyser <NUM> is shown in <FIG>, other Fourier Transform mass analysers may be employed instead. For example a Fourier Transform Ion Cyclotron Resonance (FTICR) mass analyser may be utilised as mass analyser for the MS1 scans. Mass analysers, such as the orbital trapping mass analyser and Ion Cyclotron Resonance mass analyser, may also be used in the invention even where other types of signal processing than Fourier transformation are used to obtain mass spectral information from the transient signal (see for example <CIT>, Thermo Fisher Scientific).

In a second mode of operation of the C-trap <NUM>, ions passing through the quadrupole exit lens/split lens arrangement <NUM> and first transfer multipole <NUM> into the C-trap <NUM> may also continue their path through the C-trap and into the fragmentation chamber <NUM>. As such, the C-trap effectively operates as an ion guide in the second mode of operation. Alternatively, cooled ions in the C-trap <NUM> may be ejected from the C-trap in an axial direction into the fragmentation chamber <NUM>. The fragmentation chamber <NUM> is, in the mass spectrometer <NUM> of <FIG>, a higher energy collisional dissociation (HCD) device to which a collision gas is supplied. Precursor ions arriving into the fragmentation chamber <NUM> collide with collision gas molecules resulting in fragmentation of the precursor ions into fragment ions.

Although an HCD fragmentation chamber <NUM> is shown in <FIG>, other fragmentation devices may be employed instead, employing such methods as collision induced dissociation (CID), electron capture dissociation (ECD), electron transfer dissociation (ETD), photodissociation, and so forth.

Fragmented ions may be ejected from the fragmentation chamber <NUM> at the opposing axial end to the C-trap <NUM>. The ejected fragmented ions pass into a second transfer multipole <NUM>. The second transfer multipole <NUM> guides the fragmented ions from the fragmentation chamber <NUM> into an extraction trap (second ion trap) <NUM>. The extraction trap <NUM> is a radio frequency voltage controlled trap containing a buffer gas. For example, a suitable buffer gas is argon at a pressure in the range <NUM>×<NUM>-<NUM> mBar to <NUM>×<NUM>-<NUM> mBar. The extraction trap has the ability to quickly switch off the applied RF voltage and apply a DC voltage to extract the trapped ions. A suitable flat plate extraction trap, also referred to as a rectilinear ion trap, is further described in <CIT>). Alternatively, a C-trap may also be suitable for use as a second ion trap.

The extraction trap <NUM> is provided to form an ion packet of fragmented ions, prior to injection into the time of flight mass analyser <NUM>. The extraction trap <NUM> accumulates fragmented ions prior to injection of the fragmented ions into the time of flight mass analyser <NUM>.

Although an extraction trap (ion trap) is shown in the embodiment of <FIG>, the skilled person will appreciate that other methods of forming an ion packet of fragmented ions will be equally suitable for the present invention. For example, relatively slow transfer of ions through a multipole can be used to affect bunching of ions, which can subsequently be ejected as a single packet to the TOF mass analyser. Alternatively orthogonal displacement of ions may be used to form a packet. Further details of these alternatives are found in <CIT> which describes a travelling wave ion bunching method.

In <FIG>, the time of flight mass analyser <NUM> shown is a multiple reflection time of flight mass analyser (mr-TOF) <NUM>. The mr-TOF <NUM> is constructed around two opposing ion mirrors <NUM>, <NUM>, elongated in a drift direction. The mirrors are opposed in a direction that is orthogonal to the drift direction. The extraction trap <NUM> injects ions into the first mirror <NUM> and the ions then oscillate between the two mirrors <NUM>, <NUM>. The angle of ejection of ions from the extraction trap <NUM> and additional deflectors <NUM>, <NUM> allow control of the energy of the ions in the drift direction, such that ions are directed down the length of the mirrors <NUM>, <NUM> as they oscillate, producing a zig-zag trajectory. The mirrors <NUM>, <NUM> themselves are tilted relative to one another, producing a potential gradient that retards the ions' drift velocity and causes them to be reflected back in the drift dimension and focused onto a detector <NUM>. The tilting of the opposing mirrors would normally have the negative side-effect of changing the time period of ion oscillations as they travel down the drift dimension. This is corrected with a stripe electrode <NUM> (to act as a compensation electrode) that alters the flight potential for a portion of the inter-mirror space, varying down the length of the opposing mirrors <NUM>, <NUM>. The combination of the varying width of the stripe electrode <NUM> and variation of the distance between the mirrors <NUM>, <NUM> allows the reflection and spatial focusing of ions onto the detector <NUM> as well as maintaining a good time focus. A suitable mr-TOF <NUM> for use in the present invention is further described in <CIT>).

Ions accumulated in the extraction trap are injected into the mr-TOF <NUM> as a packet of ions, once a predetermined number of ions have been accumulated in the extraction trap. By ensuring that each packet of ions injected into the mr-TOF <NUM> has at least a predetermined (minimum) number of ions, the resulting packet of ions arriving at the detector will be representative of the entire mass range of interest of the MS2 spectrum. Accordingly, a single packet of fragmented ions is sufficient to acquire MS2 spectra of the fragmented ions. This represent an increased sensitivity compared to conventional acquisition of time of flight spectra in which multiple spectra typically are acquired and summed for each given mass range segment. Preferably, a minimum total ion current (TIC) in each narrow mass window is accumulated in the extraction trap before ejection to the time of flight mass analyser. Preferably, at least N spectra (scans) are acquired per second in the MS2 domain by the time of flight mass analyser, wherein N= <NUM>, or more preferably <NUM>, or <NUM>, or more.

According to the invention, at least X% of the MS2 scans contain more than Y ion counts (wherein X= <NUM>, or <NUM>, or <NUM>, or most preferably <NUM>, or more, and Y=<NUM>, or <NUM>, or <NUM>, or <NUM>, or <NUM>, or <NUM>, or more). Most preferably, at least <NUM>% of the MS2 scans contain more than <NUM> ion counts, or more preferably more than <NUM> ion counts. This provides for an increased dynamic range of MS2 spectra. The desired ion counts for each of the MS2 scans may be provided by adjusting the number ions included in each packet of fragmented ions. For example, in the embodiment of <FIG>, the accumulation time of the extraction trap is adjusted to ensure that a sufficient number of ions have been accumulated. As such, the controller <NUM> may be configured to determine that a suitable packet of fragmented ions has been formed when either a predetermined number of ions are present in the extraction trap, or a predetermined period of time has passed. The predetermined period of time may be specified in order to ensure that the time of flight mass analyser operates at the desired frequency when the flow of ions to the extraction trap is relatively low.

The mass spectrometer <NUM> is under the control of a controller <NUM> which, for example, is configured to control the timing of ejection of the trapping components, to set the appropriate potentials on the electrodes of the quadrupole etc so as to focus and filter the ions, to capture the mass spectral data from the orbital trapping device <NUM>, to capture the mass spectral data from the mr-TOF <NUM>, control the sequence of MS1 and MS2 scans and so forth. It will be appreciated that the controller <NUM> may comprise a computer that may be operated according to a computer program comprising instructions to cause the mass spectrometer to execute the steps of the method according to the present invention.

It is to be understood that the specific arrangement of components shown in <FIG> is not essential to the methods subsequently described. Indeed other arrangements for carrying out the DIA methods of embodiments of the present invention are suitable.

An exemplary embodiment of the method will now be described with reference to <FIG> and <FIG>, in which sample molecules are supplied from a liquid chromatography (LC) column as part of the exemplary apparatus described above (as shown in <FIG>).

In the exemplary embodiment of the invention, the sample ions are supplied from the LC column such that the DIA methodology according to the present invention acquires data about the sample over a duration corresponding to a duration of a chromatographic peak of the sample supplied from the LC column. As such, the controller <NUM> is configured to perform the method within a time period corresponding to the width (duration) of a chromatographic peak at its base.

As shown in <FIG>, an orbital trapping mass analyser (denoted "Orbitrap") is utilised to perform a plurality of MS1 scans across a mass range of interest. For example, as shown in <FIG>, the mass range of interest to be analysed is <NUM>-<NUM>/z. Within the mass range of interest, a plurality of MS1 scans are performed using mass sub ranges of precursor ions of the mass range of interest. Alternatively, a single MS1 scan may be performed using precursor ions from the entire mass range of interest (i.e. <NUM>-<NUM> amu in this example).

In order to perform a single MS1 scan, sample molecules from an LC column are ionized using the ESI source <NUM>. Sample ions subsequently enter the vacuum chamber of the mass spectrometer <NUM>. The sample ions are directed by through capiliary <NUM>, RF-only lens <NUM>, injection flatapole <NUM>, bent flatapole <NUM> and into the quadrupole mass filter <NUM> in the manner as described above. The quadrupole mass filter <NUM> is controlled by the controller <NUM> to filter the sample ions according to the selected precursor mass sub-range of interest. For example, as shown in <FIG> MS1 scans are performed across a mass range of interest from <NUM>/z to <NUM>/z in precursor mass sub-ranges of <NUM>-<NUM>/z, <NUM>-<NUM>/z. to <NUM>-<NUM>/z.

Ions then pass through the quadrupole exit lens/split lens arrangement <NUM>, through the transfer multipole <NUM> and into the C-trap <NUM> where they are accumulated. From the C-trap <NUM>, (precursor) sample ions of the mass range segment may be injected in to the orbital trapping mass analyser <NUM>. Once ions are stabilised inside the orbital trapping mass analyser, the MS1 scan is performed by using the image current detector to detect the ions present in the orbital trapping mass analyser <NUM>. The detection of the ions in the orbital trapping mass analyser is configured to be performed with a relatively high resolution for the MS1 scan (relative to the resolution of the MS2 scans). For example, a resolution (R) of at least <NUM>,<NUM>, or preferably at least <NUM>,<NUM> may be used for each MS1 scan (see Resolution R=<NUM>,<NUM> in <FIG>).

By using a Fourier Transform mass analyser (for example an orbital trapping mass analyser), the MS1 scans are performed with a high degree of mass accuracy. Preferably, the MS1 scans are performed with a mass accuracy of less than <NUM>, or more preferably <NUM> parts per million (ppm). Parts per million mass accuracy Δm of a mass analyser may be determined as the difference between the measured mass of an ion mi and the actual mass of an ion ma, divided by the actual mass of the ion, multiplied by <NUM><NUM>, as shown below: <MAT>.

In tandem with the MS1 scans, a plurality of MS2 scans are performed, as shown in <FIG>. The MS2 scans are performed using a time of flight mass analyser, or more preferably a mr-TOF, as shown in <FIG>.

In order to perform a single MS2 scan of a mass range segment, sample molecules from an LC column are ionized and injected into the mass spectrometer in a similar manner to the MS1 scan. The sample ions for the MS2 scan progress through the capiliary <NUM>, RF-only lens <NUM>, injection flatapole <NUM>, bent flatapole <NUM> and into the quadrupole mass filter <NUM> in a similar manner to the sample ions for the MS1 scan.

Once the sample ions for the MS2 scan reach the quadrupole mass filter <NUM>, the quadrupole mass filter <NUM> is controlled by the controller <NUM> to filter the sample ions according to the relatively narrow mass range segment being scanned. Each precursor mass range segment has a mass range of no greater than <NUM> amu, or preferably no greater than <NUM> amu, or more preferably no greater than <NUM> amu (as shown in <FIG>).

The (filtered mass range segment) precursor ions pass from the quadrupole mass filter <NUM> through to the C-trap <NUM> as described above for the MS1 scan. The controller <NUM> then controls the C-trap to allow the precursor ions to pass through in an axial direction towards the fragmentation chamber <NUM>.

In the HCD fragmentation chamber <NUM>, the precursor ions collide with collision gas molecules which results in the fragmentation of the precursor ions into fragment ions.

The fragmented ions for the mass range segment are then ejected from the fragmentation chamber at the opposing axial end to the C-trap <NUM>. The ejected fragmented ions pass into a second transfer multipole <NUM>. The second transfer multipole <NUM> guides the fragmented ions from the fragmentation chamber <NUM> into an extraction trap (second ion trap) <NUM> where they are accumulated. The fragmented ions may be accumulated in the extraction trap <NUM> for a predetermined time.

Fragmented ions are then injected from the extraction trap injected into the mr-TOF. The prior accumulation of fragmented ions in the extraction trap allows the fragmented ions to be injected as a packet into the mr-TOF. The packet of ions travels along the flight path of the mr-TOF undergoing multiple reflections before being detected at the detector. The varying arrival times of the fragmented ions within the packet allows a MS2 mass spectrum for the packet of fragmented ions to be generated. The length of the flight path of the mr-TOF in combination with the time resolution of the detector allows the mr-TOF to perform MS2 scans at a resolution in excess of <NUM>,<NUM> (see R=<NUM>,<NUM> in <FIG>).

One benefit of the packet-based approach to the analysis of the fragmented ions in the MS2 domain, is that once the accumulated ions are ejected from the extraction trap, the fragmented ions for the next mass range segment can begin to fill the extraction trap. As such, fragmented ions from one mass range segment can be travelling through the mr-TOF while the next mass range segment of fragmented ions is being accumulated. Thus, a greater number of ion counts in each MS2 scan can be achieved within a chromatographic peak due to the use of the accumulated packet based injection of fragmented ions into the mr-TOF from the extraction trap.

According to the exemplary embodiment, in a single cycle of the DIA methodology, the controller <NUM> controls the mass spectrometer <NUM> to perform the plurality of MS1 scans of the mass sub-ranges for the mass range of interest, and in tandem the plurality of MS2 scans of the mass range segments over the mass range of interest. In order to acquire a more accurate sample of the chromatographic peak, the controller <NUM> may repeat the cycle of the DIA methodology a number of times over the duration of the chromatographic peak. For example, a single cycle of the DIA methodology may take around <NUM> to perform. As such, the cycle may be performed at least <NUM> times, or more preferably at least <NUM> times over the duration of a chromatographic peak. This enables the MS1 and/or MS2 spectral data to be used for quantitation of the eluting sample in the chromatographic peak.

A further exemplary embodiment of the method of the present invention is described in the flow chart of <FIG>. As shown in <FIG>, a plurality of MS1 and MS2 scans may be performed in tandem. In the further exemplary embodiment, sample molecules may be supplied from a liquid chromatography (LC) column, for example as part of the exemplary apparatus described above (as shown in <FIG>).

According to the further exemplary embodiment, at a time T1, precursor ions travel from the ESI <NUM> source through to the C-trap <NUM>, for example in a manner as described previously. Along the way, the precursor ions are filtered by the quadrupole mass selector <NUM> to leave ions in a first mass range segment (e.g. <NUM>-<NUM>/z).

Once the C-trap <NUM> is filled, at a time T2, precursor ions in the first mass range segment are ejected to the orbital trapping mass analyser <NUM> for performing the MS1 scan. The MS1 scan in the orbital trapping mass analyser <NUM> is performed in tandem (parallel) with the plurality of MS2 scans in the mr-TOF <NUM>. As shown, one MS1 scan in the orbital trapping mass analyser for one of the mass sub-ranges (at resolution of <NUM>,<NUM>) takes <NUM> seconds.

At a time T3, a packet of precursor ions is passed from the ESI source <NUM>, filtered through the quadrupole mass selector through the C-Trap <NUM> and to the collision cell. The quadrupole mass selector <NUM> filters the ions to define a first mass range segment (e.g. <NUM>-<NUM>/z as shown in <FIG>). Effectively, the C-Trap <NUM> operates as an ion guide except at times T1 and T2.

At a time T4, the first mass range segment of precursor ions are then sent to the collision cell <NUM>, where they are fragmented. The fragmented ions are then sent onwards to the mr-TOF <NUM> where they are accumulated in the extraction trap <NUM>.

At a time T5, the extraction trap <NUM> ejects a packet of fragmented ions for travel along the flight path.

At a time T6, the mr-TOF <NUM> detects the fragmented ions at the detector <NUM>. As shown, one MS2 scan in the time of flight mass analyser for one of the mass range segments (at resolution of <NUM>,<NUM>, <NUM>) takes <NUM> milliseconds. According to the embodiment of <FIG>, although the MS2 scan takes <NUM> to perform, the time taken to fragment the ion (<NUM>), and accumulate the ions in the extraction trap and eject them (<NUM>) takes a total time period of <NUM>. Accordingly the time period for performing a single MS2 scan according to this embodiment is set by this <NUM> time period. In other embodiments, the time for performing these method steps may be varied in order to vary the frequency of performing the MS2 scans.

At a time T7, a subsequent set of precursor ions is filtered to using the next narrow mass window for the next MS2 scan (i.e. mass range <NUM>-<NUM>/z), fragmented in the collision cell (time T8), ejected from the extraction trap (time T9) and detected at the detector (time T10). As such, the DIA apparatus processes multiple packets of ions for the MS2 scans at once at different points in the system. For example, the extraction trap is being filled with ions whilst the previous ion packet is flying through the mr-TOF <NUM>. As such, the parallel TOF MS2 acquisition step is performed concurrently with the steps of fragmenting the ions and accumulating the ions for ejection into the TOF. In some embodiments, it is preferable that whilst fragmented ions are cooling in the extraction trap <NUM> a further ion packet should be fragmenting in the collision cell <NUM>.

Thus, as shown in <FIG>, MS2 scans are performed for each narrow mass window across the precursor mass sub-range (e.g. <NUM>-<NUM>/z).

Once the MS1 scan and the plurality of MS2 scans for the mass sub-range <NUM>-<NUM>/z are complete, the MS1 scan and MS2 scans above are repeated for the next mass sub-range (e.g. <NUM>-<NUM>/z). Accordingly, in the exemplary embodiment of <FIG>, performing the MS1 scan and plurality of MS2 scans for each mass sub-range takes <NUM>. Thus, the complete DIA scan of the mass range of interest may be completed in a cycle time of <NUM>. By performing a high resolution, high mass accuracy DIA methodology with a cycle time of <NUM>, the DIA methodology of the present invention may be performed a number of times over the duration of a chromatographic peak. For example, the method of the present invention may be repeated at least: <NUM>, <NUM>, <NUM>, <NUM>,or more preferably at least <NUM> times across the duration of the chromatographic peak. Thus, a chromatographic peak may be fully sampled using a DIA methodology according to the present invention.

The precursor ion spectra acquired at high resolution and high mass accuracy in the orbital trapping mass analyser can be used to produce a precursor ion candidate list using a standard non-fragment ion-database. In-silico fragmentation of the candidates in the list produces within the narrow mass range of interest a library against which fragmentation spectra are compared and/or quantified as known in the art in order to provide identification of the precursor ions.

The skilled person will understand from <FIG>, that the DIA methodology of the present invention may be applied to any mass range of interest. For example, a mass range of interest may include a mass to charge ratio of at least: <NUM>, <NUM>, <NUM>, <NUM>, <NUM> or <NUM>/z in order to analyse precursor ions of a relatively small m/z. A mass range of interest may also include a mass to charge ratio of up to: <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM> or <NUM>/z in order to analyse precursor ions of a relatively large m/z.

In one alternative embodiment, a set of MS2 scans may be acquired by multiplexing precursor ions from a plurality of different mass range segments in a single MS2 analysis. In this alternative method of performing a set of MS2 scans, the MS1 scans may be acquired according to any of the methodologies described previously.

In the alternative embodiment, for each MS2 scan making up the set of MS2 scans, a plurality of mass range segments are selected. A different combination of mass range segments is selected for each scan in the set of MS2 scans, and also ensures that every mass range segment is selected at least once. In the alternative embodiment, precursor ions from the selected combination of mass range segments may be fragmented and analysed together as part of a single MS2 scan. The precursor ions in each mass range segment may be fragmented separately and the resulting fragmented ions formed (accumulated) into a packet together to be scanned together in the TOF mass analyser. Alternatively, the precursor ions in the plurality of mass range segments to be combined may be fragmented together, and then scanned together in the TOF mass analyser. For example, a first MS2 scan may be performed on precursor ions from mass range segments with mass to charge ratios of <NUM>-<NUM>, <NUM>-<NUM> and <NUM>-<NUM>. A second MS2 scan may then be performed on a different combination of mass range segments. Once all the MS2 scans in the set have been performed, the MS2 data may be deconvoluted in order obtain data suitable for identification and/or quantitation of the sample. Further details of the methodology and the deconvolution process may be found in "<NPL>.

In a further alternative embodiment, the mass spectrometer according to the present invention may be provided in a branched path arrangement, for example as shown in the embodiment in <FIG>. In the embodiment of <FIG>, an ion source <NUM> is coupled to a mass selection device <NUM>. Such an arrangement may be provided by the ESI ion source <NUM> and its respective couplings to the quadrupole mass filter <NUM> as shown in the embodiment of <FIG> for example.

As shown in <FIG>, the output of the mass selection device <NUM> is coupled to the branched ion path <NUM>. The branched ion path directs ions output from the mass selection device along one of two paths. A first path <NUM> directs ions to a C-trap <NUM> where ions are collected for analysis by a Fourier Transform mass analyser, for example an orbital trapping mass analyser <NUM> in the MS1 domain. A second path <NUM> directs ions to a fragmentation chamber <NUM> for fragmentation of ions and subsequent mass analysis in the MS2 domain. The branched ion path may use an rf voltage to direction ions down either the first path <NUM> or the second path <NUM>. The branched ion path may be a branched RF multipole. A branched ion path suitable for use in the embodiment of <FIG> is further described in <CIT>.

According to the alternative embodiment in <FIG>, the branched ion path may be used to direct ions to a C-trap <NUM> for MS1 analysis or to a fragmentation chamber <NUM> for MS2 analysis. Fragmented ions ejected from the fragmentation chamber <NUM> may be accumulated in ion extraction trap <NUM>, before being injected into mr-TOF analyser <NUM> as a packet. As such, the arrangement of the fragmentation chamber <NUM>, ion trap <NUM> and mr-TOF <NUM> may be provided by a similar arrangement as described in <FIG>.

Thus, according to the alternative embodiment in <FIG>, ions may be directed for MS2 analysis without requiring the C-trap <NUM> supplying the MS1 orbital trapping mass analyser <NUM> to be empty. Such a configuration may allow increased parallelisation of the MS1 and MS2 scans. As such, a greater proportion of the duration of a chromatographic peak may be available for carrying out MS2 scans. Furthermore, in this configuration, a number of loadings or fills can be accumulated in the C-trap <NUM> before analysis in the orbital trapping mass analyser <NUM>, as shown in <FIG>, which are discussed further below. In such embodiments, the loading (filling) of the C-trap <NUM> can be split into several small fills whilst the orbital trap mass analyser <NUM> is scanning, thereby to obtain a population of ions that is more representative of the ions from across the entire peak.

<FIG> show schematic diagrams of a method of DIA analysis using the branched path configuration of the mass analysers. <FIG> shows a representation of a chromatographic peak of a sample as it elutes from a chromatographic apparatus. The dots superimposed on the peak represent time periods in which an MS1 scan is started, while the lines are representative time periods in which individual MS2 scans are performed. As such, the dots correspond to starting points for separate cycles of the DIA methodology.

By utilising the branched path arrangement, the C-trap <NUM> is no longer in the path of the supply of ions to the fragmentation chamber for performing the MS2 scans. Accordingly, the C-trap <NUM> according to the branched path embodiment may be loaded over an extended time period using a plurality of smaller filling steps.

<FIG> shows a schematic representation of the operation of the C-trap and Orbitrap over time for performing MS1 scans according to the embodiment of <FIG>. The axis denoted "orbi LT "represents the ion flow into the C-trap <NUM> over time, while the axis denoted "orbitrap" represents the operation of the orbital trapping mass analyser for performing an MS1 scan over time. As shown in <FIG>, ions flow into the C-trap <NUM> at a number of relatively short periods over the duration of an MS1 scan by the orbital trapping mass analyser. As such, the C-trap <NUM> is filled using a plurality of fills distributed over a period of time corresponding to the duration of an MS1 scan. As such, in a sequence of MS1 scans, the ions for the following MS1 scan are loaded into the C-trap <NUM> while the current MS1 scan is performed. Advantageously, by loading the C-trap <NUM> in this manner, the ions in the C-trap <NUM> may be more representative of the sample over the duration of loading.

As further shown in <FIG>, the loading of the C-trap <NUM> is performed in parallel with the performance of the loading of the extraction trap for the MS2 scans. The axis in <FIG> denoted "TOF LT" represents the ion flow into the extraction trap <NUM> over time. The axis denoted "TOF" in <FIG> represents the operation of the TOF mass analyser performing MS2 scans over time. As shown in <FIG>, each filling of the extraction trap has a corresponding MS2 scan. The skilled person will appreciate that the graph is not to scale and is not intended to accurately represent the relative frequencies of the performance of the MS1 and MS2 scans.

A further alternative embodiment of the invention is disclosed in <FIG> depicts a schematic diagram of a tandem mass spectrometer <NUM> including an orbital trapping mass analyser <NUM> and a time of flight mass analyser <NUM> in a branched path configuration.

The embodiment in <FIG> includes an ion source <NUM> and ion guide <NUM> which supply precursor ions to a mass selector <NUM>. Such an arrangement may be provided by the ESI ion source <NUM> and its respective couplings to the quadrupole mass filter <NUM> as shown in the embodiment of <FIG> for example.

As shown in <FIG>, a branched ion path <NUM> guides ions from the mass selector <NUM> to a C-trap <NUM> and/or an extraction trap <NUM>. The C-trap <NUM> supplies ion to the orbital trapping mass analyser <NUM> for MS1 scans, while the extraction trap <NUM> supplies ions to the time of flight mass analyser <NUM>. For example, a similar arrangement to the embodiment disclosed in <FIG> may be provided.

<FIG> additionally includes a dual linear trap <NUM>,<NUM>. The dual linear trap is connected downstream of the C-trap <NUM> between the C-trap <NUM> and the extraction trap <NUM> for the time of flight mass analyser. The dual linear trap may be connected to the C-trap <NUM> and the extraction trap <NUM> by ion guides <NUM>, <NUM>. Ion guide <NUM> may be a branched ion path which merges with the ion path from the mass selector <NUM> in order to connect to the extraction trap <NUM>.

The dual linear trap <NUM>, <NUM> may be provided for fragmentation and/or mass isolation of the ions. For example, a first ion trap <NUM> may be provided as a high energy collision dissociation chamber. A second ion trap, downstream of the first ion trap may be provided as a low collision dissociation chamber. By including a second dissociation chamber, fragmented ions may readily be fragmented again in the second chamber in order to perform MS3 analysis. Ions may be repeatedly isolated and fragmented for MSn analysis. The dual linear trap may also allow for fragmentation by collision induced dissociation (CID), electron capture dissociation (ECD), electron transfer dissociation (ETD), ultraviolent photo dissociation (UVPD), and so forth. Further details of a suitable dual ion trap may be found in <CIT>.

Advantageously, by providing a branched path directly to the extraction trap <NUM> from the mass selector <NUM>, ions may be more efficiently transferred from the mass selector <NUM> to the extraction trap.

The above described mass spectrometers may also be well suited to carrying out the DIA methodologies described in <CIT> (published as <CIT>) , wherein the MS2 scans are performed using the time of flight analyser of the above described mass spectrometers, and MS1 scans are performed using the above described orbital trapping mass analysers.

It will be appreciated that other embodiments of ion injection into the time of flight mass analyser may be used in place of the extraction trap, although they may not be as advantageous. For example, an orthogonal accelerator may be used to inject packets of ions into the time of flight mass analyser. However, the ion counts in each MS2 spectrum, and thus dynamic range and sensitivity, in such embodiments will typically be lower than can be obtained using the extraction trap to accumulate ions before each injection into the time of flight mass analyser. In a further alternative embodiment, a slow transfer multipole may be used in place of the extraction trap to inject packets of ions into the time of flight mass analyser. In this way, ions may be bunched in the multipole (and not lost) before each packet is injected into the TOF analyser.

Advantageously, the present invention may be used to create a high resolution, high mass accuracy DIA workflow, which can deliver high confidence of identification, and better precision of quantitation than approaches previously known in the art. In some embodiments, the present invention is capable of delivering <NUM> % identification of all detectable features in a sample in the MS1 level and with a higher degree of sensitivity than quantitation in the MS2 level, as quantitation is performed prior to fragmentation of the sample precursors (i.e. with unfragmented precursors). For example, quantitation of precursor ions may be performed in the MS1 domain using a "library free" approach, thus reducing the requirements on post-processing of the acquired data. One method for analysing DIA MS1 scan data and quantitating precursor ions using a library free approach is described in "<NPL>.

For successful identification of precursor ion information by the methodology of the present invention, the MS1 scans are performed with a resolution of preferably at least <NUM>,<NUM>, or more preferably at least <NUM>,<NUM>, or better still at least <NUM>,<NUM> and preferably <NUM>-2ppm or better in mass accuracy, while in the ion fragment (MS2) spectra at least <NUM>,<NUM> or more preferably at least <NUM>,<NUM> resolution and preferably <NUM>-<NUM> ppm or better mass accuracy is preferable.

Claim 1:
A data independent acquisition method of mass spectrometry for analysing a sample within a mass range of interest, the method being performed within a time period based on a width of a chromatographic peak of the sample as it elutes from a chromatography system and comprising the steps of:
ionising the sample to produce a plurality of precursor ions;
selecting precursor ions within a mass range of interest to be analysed;
performing at least one MS1 scan of the precursor ions comprising:
mass analysing precursor ions across the mass range of interest using a first mass analyser, for identification and/or quantitation of the precursor ions in the MS1 domain, wherein the first mass analyser is a Fourier Transform mass analyser, an orbital trapping mass analyser (<NUM>), an ion cyclotron resonance (ICR) mass analyser, or a time of flight mass analyser; and
performing a set of MS2 scans, the set of MS2 scans comprising:
segmenting the precursor ions into a plurality of precursor mass segments, each precursor mass segment having a mass range of no greater than <NUM> amu;
wherein for each precursor mass segment:
fragmenting the precursor ions within that precursor mass segment; and
performing an MS2 scan of the fragmented ions by:
accumulating the fragmented ions, forming an ion packet from the accumulated fragmented ions; and injecting the ion packet of fragmented ions into a time of flight mass analyser (<NUM>) and mass analysing the fragmented ions;
wherein at least X% of the MS2 scans contain more than Y ion counts, wherein X= <NUM>, or <NUM>, or <NUM>, or <NUM>, and Y= <NUM>, or <NUM>, or <NUM>, or <NUM>, or <NUM>;
wherein accumulating fragmented ions comprises accumulating fragmented ions in an ion trap for a predetermined time; and
wherein the predetermined time for accumulating fragmented ions is adjusted to accumulate a sufficient number of ions such that the at least X% of the MS2 scans contain more than Y ion counts.