Patent Description:
It is known to mass selectively eject ions from an ion trap into a pusher region of a time of flight (ToF) mass analyser so as to time focus a given range of mass to charge ratios within the pusher and hence increase the duty cycle of the analyser. It is also known to use an ion mobility separator to temporally separate ions upstream of a ToF mass analyser, and then synchronise the pusher of the ToF analyser with the arrival times of the ions from the ion mobility separator. However, this method is generally only suitable for use with ions of a single charge state, as the ion mobility separation results in the temporal separation of ions of different charge states. It is also known to release ions from a small, low resolution TOF region into a travelling wave ion guide. The velocity of the travelling wave along the ion guide is controlled such that the required mass ranges may be separated temporally and introduced into the pusher region of a TOF mass analyser so as to increase the duty cycle of the mass analyser. However, the velocity requirements for the travelling wave may result in significant fragmentation of ions at low mass to charge ratios. It is desired to provide and improved method and apparatus for improving the duty cycle of a discontinuous ion analyser such as a time of flight (ToF) mass analyser.

Document <CIT> discloses an ion trap in which ions are trapped along the axis of the trap at a location that is dependent on their mobility due to a balance between a force from a gas flow towards the exit of the trap and a force from an electric potential gradient with its highest potential near the exit of the trap. As the gradient is reduced, the gas flow will push the lowest mobility ions out of the trap, while the remaining ions are redistributed closer to exit of the trap.

The present invention provides a method of mass spectrometry and/or ion mobility spectrometry as claimed in claim <NUM>.

It will be appreciated that a discontinuous ion analyser is an ion analyser that analyses ions in a sequence of cycles, rather than continuously. For example, a Time of Flight mass analyser is a discontinuous ion analyser that receives ions in an ion extraction region and periodically pulses them into the time of flight region to a detector for mass analysis. Each pulse to the detector is a separate cycle of analysis.

Conventional arrangements may store ions in an ion trap upstream of a discontinuous ion analyser and then pulse all of the ions from the ion trap into the ion analyser in a single pulse. Using such an ion trap may improve the duty cycle of the instrument, for example, by converting a continuous ion beam into a pulsed ion source. However, if the ions in the ion trap have a relatively wide range of physicochemical property values then they may not all be able to be analysed in the same cycle by a discontinuous ion analyser, resulting in a lower duty cycle. For example, when a group of ions having a wide range of mass to charge ratios is pulsed into a ToF mass analyser, the ions of different mass to charge ratio spread temporally such that not all of the ions are present in the pusher region when the extraction pulse is applied. This leads to a lower duty cycle. Also, conventional methods of trapping ions upstream of the ion analyser lead to detrimental space-charge effects.

The present invention enables a population of ions having a relatively broad range of physicochemical property values (e.g. mass to charge ratios) to be stored in an ion trap and analysed in a discontinuous analyser, whilst maintaining a high duty cycle. In particular, by separating ions within the ion trap according to a physicochemical property and driving ions out of the ion trap from different regions at different times, the ion analyser receives ions having a relatively small range of physicochemical property values in each analysis cycle. The technique also has relatively low space-charge effects, as the ions are spatially separated within the ion trap.

<CIT> discloses a mass selective ion trap that is synchronised with a scanned mass filter. Pseudo-potential corrugations may be formed along the length of the ion trap and an axial field may be used to drive ions against these corrugations. As ions of different mass to charge ratios experience different forces from the pseudo-potential corrugations, ions may be ejected in reverse order of mass to charge ratios by sweeping the RF potentials applied to the ion trap. Ions are therefore mass selectively scanned out of the ion trap as a continuous stream. However, until the ions are ejected they remain trapped together and are not spatially separated within the ion trap according to a physicochemical property so that ions having different values of the physicochemical property are trapped in different regions of the ion trap. As such, the space-charge effects in WO'<NUM> remain relatively high. Also, the instrument is unable to eject pulses of ions from the different regions of the ion trap in order to eject ions having different ranges of physicochemical property, since in WO'<NUM> the different ions are trapped together in the same trapping region.

<CIT> discloses a series of ion traps. Ions of different mass to charge ratios may be ejected through a slot in an electrode of each ion trap at different times by scanning the trapping voltages. However, this instrument does not spatially separate the ions within a trap so that ions of different values of a physicochemical property are trapped in different regions of the trap. Rather, it would seem that the different ions would intermix as they oscillate in the RF trapping fields. Also, the instrument does not analyse ions ejected from different trapping regions in different cycles of a discontinuous analyser. There would seem to be no need to pulse ions into a discontinuous analyser in the instrument of EP'<NUM> since a continuous detector may be used in combination with the extraction voltages to determine the mass to charge ratios of the ions. The concept described above of enhancing the duty cycle in a discontinuous analyser is not suggested in EP'<NUM>.

<CIT> discloses a plurality of ion guiding channels in which pseudo-potential wells are arranged that manipulate ions in a number of ways. This instrument may lower the potential barrier between adjacent wells in order to separate ions according to mass to charge ratio, although the separated ions are not then pulsed into a discontinuous ion analyser in different cycles of the analyser. This instrument may also be used to mass selectively eject ions from a pseudo-potential well at the end of an ion guiding channel, although this technique is similar to the ion trap in <CIT> in that different ions are not trapped in different regions of the well and there is no requirement to use a discontinuous analyser.

According to embodiments of the present invention, said step of driving or pulsing second trapped ions out of the second region of the ion trap may be performed whilst retaining other ions trapped in the ion trap.

The ions may be spatially separated within the ion trap according to the at least one physicochemical property so that the ions are dispersed along the ion trap according to their physicochemical property values without the spatially separated trapped ions being separated by potential barriers. The step of spatially separating the ions may not therefore comprise arranging a potential barrier, such as a DC potential barrier, between the ions of different physicochemical property values. In this context, such a potential barrier is intended to mean a discrete barrier or well, rather than a potential gradient.

Whilst the first and/or second trapped ions are driven or pulsed out of the first and/or second regions of the ion trap, the other trapped ions may be caused to remain trapped at their respective different trapping regions, optionally until said other trapped ions are driven or pulsed out of their respective trapping regions into the discontinuous ion analyser.

Accordingly, whilst the first trapped ions are driven or pulsed out of the first region of the ion trap, the second trapped ions may be caused to remain in said second region until the second trapped ions are driven or pulsed out of the second region into the discontinuous ion analyser at the second time.

The first region may be closer to the exit of the ion trap than the second region.

Although first and second trapped ions have been described as being trapped and then driven or pulsed out of first and second trapping regions, further groups of ions may also be trapped in further trapping regions and then driven or pulsed out of those further trapping regions into the ion analyser. Accordingly, the method may comprise performing one or more further cycle of operation, wherein each cycle comprises: driving or pulsing trapped ions out of a region of the ion trap and into the discontinuous ion analyser, whilst retaining other ions trapped in the ion trap, and analysing the ions driven or pulsed out of the ion trap in a cycle of said discontinuous ion analyser; wherein for each subsequent cycle of operation, ions are driven or pulsed out of a different region of the ion trap from the previous cycles of operation, and the ions that are driven or pulsed out of the ion trap are analysed in a different cycle of said discontinuous ion analyser.

For each subsequent cycle of operation, ions may be driven out of the ion trap from a trapping region that is further away from the ion analyser than the region from which ions were driven out in the previous cycle of operation (e.g. further from the exit of the ion trap).

Optionally, after said step of trapping the ions, ions are not admitted into the ion trap until after said steps of driving said first and second ions out of the ion trap have been performed. Furthermore, ions may not be admitted into the ion trap until after said plurality of cycles of operation have been performed.

The method may comprise spatially separating the ions only after all of the ions to be analysed in the ion analyser have been accumulated. Alternatively, the step of spatially separating the ions may be performed whilst the ions are being accumulated in the ion trap.

The ion trap may comprise an elongated ion trapping volume, and ions having said different values of said physicochemical property may be trapped in different regions along the longitudinal axis of the ion trap. Alternatively, or additionally, the ions having said different values of said physicochemical property may be trapped in the ion trap at different distances from an entrance to the ion analyser prior to being driven out of the ion trap.

The ion trap may comprise an elongated ion guide having a plurality of electrodes arranged along its longitudinal axis. This allows different AC and/or DC voltages to be applied at different axial locations of the ion trap, for example, in order to apply the DC gradient and/or pseudo-potential and/or travelling potential described herein.

The ion trap may comprise a plurality of apertured electrodes within which the ions are trapped by application or AC and/or DC voltages to the electrode. For example, the ion trap may comprise a stacked ring ion guide or an ion tunnel ion guide. Less preferably, the ion trap may comprise one or more multipole rod sets.

The ion trap may comprise geometries of electrodes other than those described above.

The at least one physicochemical property may be mass to charge ratio and/or ion mobility.

Said step of spatially separating the ions comprises applying a first force on the ions within the ion trap in a first direction, said force having a magnitude that is dependent upon the value of said at least one physicochemical property of the ions; and applying a second force on these ions in the opposite direction. Optionally, the magnitude of said second force is not dependent upon the value of said at least one physicochemical property of the ions. Said first and second forces are counterbalanced at different locations within the ion trap for ions having different physicochemical property values, such that different ions are trapped at said different regions.

Said ion trap may comprise one or more electrodes and said method may comprise generating said first force by applying AC or RF potentials to said electrodes so as to generate a pseudo-potential electric field that urges ions in the first direction.

The ion trap may comprise one or more electrodes and said method may comprise generating said second force by applying one or more DC potentials to said one or more electrodes so as to generate a DC voltage or DC voltage gradient that urges ions in the second direction; and/or a gas flow may be provided through the ion trap so as to generate said second force.

When said step of spatially separating the ions comprises separating the ions according to more than one physicochemical property, the ions may be separated so that ions having different combinations of values for said more than one physicochemical property are trapped at different locations within the ion trapping region.

Each of the steps of driving or pulsing trapped ions out of a region of the ion trap and into a discontinuous ion analyser, whilst retaining other ions trapped in the ion trap, may comprise travelling an electric potential along at least a portion of the ion trap so as to drive the ions out of the ion trap.

The electric potential may be travelled along a first length of the ion trap in order to drive said first ions out of the ion trap, and said electric potential may be subsequently travelled along a second, different length of the ion trap in order to drive said second ions out of the ion trap.

The first and second lengths of the ion trap may be overlapping. The first length may be shorter than the second length, and the second length may include at least part of the first length.

The first length may extend from a first location in the ion trap to the exit of the ion trap, whereas the second length may extend from a second location in the ion trap to the exit of the ion trap, wherein the second location is further from the exit than the first location.

The electric potential may be travelled along third and further lengths of the ion trap in order to drive ions out of the ion trap in the one or more further cycles of operation. Optionally, in each cycle of operation the electric potential travels from an upstream location of the ion guide towards the exit of the ion guide, and wherein the upstream location becomes progressively further upstream in subsequent cycles of operation.

The electric potential that is travelled along the ion guide may be a DC potential barrier or well.

Rather than using a travelling potential to drive ions out of the ion trap in each cycle of operation, one or both of the opposing forces on the ions may be varied with time such that the resulting overall force causes ions to exit the ion guide and enter the discontinuous ion analyser in each cycle of operation. For example, the DC gradient, gas flow rate, or pseudo-potential may be changed to eject different ions in the different cycles of operation.

The discontinuous ion analyser may be a time of flight mass analyser, a pulsed ion mobility analyser, or an Orbitrap (RTM) mass analyser.

The ion analyser may be an orthogonal acceleration time of flight mass analyser. However, the ion analyser may be a linear acceleration time of flight mass analyser. The present invention is also applicable to other types of discontinuous ion analyser.

The method may comprise pulsing the ions into the ion trap before the step of separating the ions.

Substantially all of the ions driven out of the ion trap from any given trapping region may be analysed in a single cycle of the discontinuous ion analyser.

Ions having different values, or different ranges of values, for said at least one physicochemical property may be analysed in said ion analyser in different cycles.

The present invention also provides a mass spectrometer and/or ion mobility spectrometer as claimed in claim <NUM>.

The spectrometer may be arranged and configured to perform any one of the methods described herein.

For example, the ion driving device may be arranged and configured to travel an electric potential along at least a portion of the ion trap so as to drive or pulse ions out of the ion trap; and the controller may be configured to control the ion driving device such that an electric potential is travelled along a first length of the ion trap in order to drive or pulse said first ions out of the ion trap, and an electric potential is travelled along a second length of the ion trap in order to drive or pulse said second ions out of the ion trap.

The discontinuous ion analyser may be a time of flight mass analyser, or a pulsed ion mobility analyser.

Embodiments comprise pulsing ions into an ion trap, and then spatially separating the trapped ions using a combination of opposing DC and pseudo-potential fields. After separation, ions may be extracted from a selected region of the ion trap by travelling a DC potential barrier along the selected region to the exit of the ion trap, so as to urge ions out of the ion trap. The other ions remain trapped in the ion trap. The travelling potential therefore extracts ions from a given spatial range and the ions may be conditioned before passing to the pusher region of a ToF mass analyser. The pusher region pulses these ions into the ToF region and mass analyses them. A travelling potential then sweeps ions out of a different region of the ion trap and into the pusher region of the ToF mass analyser. When these ions are within the pusher region they are pulsed into the ToF region and mass analysed. The process of sweeping ions out of different regions of the ion trap and pulsing them into the ToF region is repeated.

Once ions are pulsed into the ion trap, a period of time is needed to allow the ions to spatially separate. A quantity of time is also required for the ToF mass analysis itself. This time may be used, for example, to analyse incoming ions with a different analyser, e.g. by fragmenting the ions and analysing them in an analytical ion trap.

In the method or spectrometer according to the various embodiments of the present invention, the ions of different physicochemical property values may be spatially separated over a length of ≥ x mm within the ion trap, wherein x is selected from the group consisting of: <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM> and <NUM>.

Ions having any given value for said physicochemical property may be distributed over ≤ y mm within the ion trap, wherein y is selected from the group consisting of: <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, <NUM>, and <NUM>.

Any one of the above ranges for x mm may be combined with any one of the above ranges for y mm. Both of these distances are measured along the axis of separation (i.e. the z-direction). It is desired that the range of ions is separated over a relatively large distance x mm, but that ions of any given value for said physicochemical property are distributed over a relatively small distance y mm.

Optionally, the physicochemical property value may be mass to charge ratio, the ions may be separated such that they are dispersed over a length L in the ion trap, and the ratio of the range of mass to charge ratios, in Daltons, trapped in the ion trap over length L to the length L over which the ions are trapped, in mm, may be selected from the group consisting of: (i) <NUM>-<NUM>; (ii) <NUM>-<NUM>; (iii) <NUM>-<NUM>; (iv) <NUM>-<NUM>; (v) <NUM>-<NUM>; (vi) <NUM>-<NUM>; (vii) <NUM>-<NUM>; (viii) <NUM>-<NUM>; (ix) <NUM>-<NUM>; (x) <NUM>-<NUM>; (xi) <NUM>-<NUM>; (xii) <NUM>-<NUM>; (xiii) <NUM>-<NUM>; (xiv) <NUM>-<NUM>; and (xv) <NUM>-<NUM>.

The separation of the ions according to said physicochemical property may be preserved during ejection of the ions from the ion trap.

The spectrometer described herein may comprise:.

The spectrometer may comprise an electrostatic ion trap or mass analyser that employs inductive detection and time domain signal processing that converts time domain signals to mass to charge ratio domain signals or spectra. Said signal processing may include, but is not limited to, Fourier Transform, probabilistic analysis, filter diagonalisation, forward fitting or least squares fitting.

The spectrometer may comprise a device arranged and adapted to supply an AC or RF voltage to the electrodes. The AC or RF voltage preferably has an amplitude selected from the group consisting of: (i) < <NUM> V peak to peak; (ii) <NUM>-<NUM> V peak to peak; (iii) <NUM>-<NUM> V peak to peak; (iv) <NUM>-<NUM> V peak to peak; (v) <NUM>-<NUM> V peak to peak; (vi) <NUM>-<NUM> V peak to peak; (vii) <NUM>-<NUM> V peak to peak; (viii) <NUM>-<NUM> V peak to peak; (ix) <NUM>-<NUM> V peak to peak; (x) <NUM>-<NUM> V peak to peak; and (xi) > <NUM> V peak to peak.

The AC or RF voltage preferably has a frequency selected from the group consisting of: (i) < <NUM>; (ii) <NUM>-<NUM>; (iii) <NUM>-<NUM>; (iv) <NUM>-<NUM>; (v) <NUM>-<NUM>; (vi) <NUM>-<NUM>; (vii) <NUM>-<NUM>; (viii) <NUM>-<NUM>; (ix) <NUM>-<NUM>; (x) <NUM>-<NUM>; (xi) <NUM>-<NUM>; (xii) <NUM>-<NUM>; (xiii) <NUM>-<NUM>; (xiv) <NUM>-<NUM>; (xv) <NUM>-<NUM>; (xvi) <NUM>-<NUM>; (xvii) <NUM>-<NUM>; (xviii) <NUM>-<NUM>; (xix) <NUM>-<NUM>; (xx) <NUM>-<NUM>; (xxi) <NUM>-<NUM>; (xxii) <NUM>-<NUM>; (xxiii) <NUM>-<NUM>; (xxiv) <NUM>-<NUM>; and (xxv) > <NUM>.

The spectrometer may comprise a chromatography or other separation device upstream of an ion source. The chromatography separation device may comprise a liquid chromatography or gas chromatography device. The separation device may comprise: (i) a Capillary Electrophoresis ("CE") separation device; (ii) a Capillary Electrochromatography ("CEC") separation device; (iii) a substantially rigid ceramic-based multilayer microfluidic substrate ("ceramic tile") separation device; or (iv) a supercritical fluid chromatography separation device.

The ion guide may be maintained at a pressure selected from the group consisting of: (i) < <NUM> mbar; (ii) <NUM>-<NUM> mbar; (iii) <NUM>-<NUM> mbar; (iv) <NUM>-<NUM> mbar; (v) <NUM>-<NUM> mbar; (vi) <NUM>-<NUM> mbar; (vii) <NUM>-<NUM> mbar; (viii) <NUM>-<NUM> mbar; and (ix) > <NUM> mbar.

Analyte ions may be subjected to Electron Transfer Dissociation ("ETD") fragmentation in an Electron Transfer Dissociation fragmentation device. Analyte ions may be caused to interact with ETD reagent ions within an ion guide or fragmentation device.

Various embodiments of the present invention will now be described, by way of example only, and with reference to the accompanying drawings in which:.

Embodiments of the present invention provide a method and apparatus for improving the analysis of ions in a discontinuous ion analyser by trapping ions in an ion trap, spatially separating the ions within the ion trap according to their mass to charge ratios, and then driving or pulsing ions out of different regions of the ion trap into the discontinuous ion analyser at different times.

The embodiments described herein separate the ions within an ion trap according to mass to charge ratios. The ions may be spatially separated within the ion trap using a combination of a pseudo-potential electric field and a DC electric field. For example, the ion trap may comprise a stacked ring ion guide (or other ion guide) and a controller and related electronic circuitry may control a voltage supply to apply an axial DC voltage Vdc(z) along the length of the ion trap having the following profile: <MAT> where z is the distance from the end of the ion trap, and d<NUM> and d<NUM> are the coefficients of the linear and quadratic terms.

Similarly, the controller and related electronic circuitry may control a voltage supply to apply RF voltages to the electrodes so that the RF voltage function along the ion trap, Vx(z), is as follows: <MAT> Where p<NUM> and p<NUM> are the coefficients of the linear and quadratic terms.

This results in an axial pseudo-potential profile, Vps(z,m), given by: <MAT> where M is the atomic mass unit, m is the mass to charge ratio of a given ion, and ω is the applied RF voltage frequency.

Let <MAT> Therefore, the pseudo-potential generated along the ion trap is given by: <MAT> The total potential for a given mass to charge ratio m and distance z from the end of the ion trap, Vtot, is simply the sum of VDC and Vps, and is therefore given by: <MAT>.

Ions of any given mass to charge ratio m will be located at a distance z from the end of the ion trap, at a distance where Vtot is a minimum for that mass. Differentiating equation <NUM> and solving for the minima gives equation <NUM> below: <MAT> This equation can be used to calculate the position z at which the pseudo-potential minimum for any given ion is located, and hence the position at which that ion will remain trapped.

For example, the curvature C(m) of the minima may be calculated from the second differential with respect to z of Vtot in equation <NUM>, giving: <MAT>.

As long as the value of C(m) is greater than zero then equation <NUM> gives the position of the minimum at which ions of a given mass to charge ratio will be trapped.

By optimisation of the DC potential parameters, d<NUM> and d<NUM>, and the RF potential parameters, p<NUM> and p<NUM>, it is possible to obtain reasonable voltage levels and good spatial separation of the ions within the ion trap.

This ion trap is used to separate ion according to a physicochemical property (e.g., mass to charge ratio) in the embodiments described herein.

A first set of arrangements that do not have all of the features of the independent claims will now be described, in which the ion trap is used in an ion filter which selectively ejects ions from one or more sections of the ion trap so that ions having only the desired values of a physicochemical property (e.g., mass to charge ratio) are onwardly transmitted.

As described above, with optimisation of the DC potential parameters, d<NUM> and d<NUM>, and the RF potential parameters, p<NUM> and p<NUM>, it is possible to obtain reasonable voltage levels and good spatial separation of the ions within the ion trap. In the description below the optimisation of the parameters assumes an ion trap length of <NUM> and a distribution of ions in the trap for ions having a range of mass to charge ratios of <NUM> to <NUM> Da.

<FIG> shows a graph of the position z at which the total potential Vtot is minimum as a function of ion mass to charge ratio, for ions of mass to charge ratio m between <NUM> and <NUM> Da and for optimised values of d<NUM>= -<NUM> and d<NUM>= -<NUM> which give a maximum Vdc = -<NUM> V; and p<NUM>= -<NUM> and p<NUM>=-<NUM> which give a maximum Vx = <NUM> V, ω = <NUM>.

The ions are cooled by a buffer or background gas in the ion trap and they reach thermal energy. A worst case assumption would be that the residual axial energy ΔV of the ions was approximately ten times this value, say ΔV= <NUM> eV. This assumption then allows the spatial width Δz(m) along the z-direction of the ion trap that any given ion will reside within to be determined, i.e. +/-<NUM> V from the central potential position.

The spatial width Δz(m) along the ion trap in the z-direction within which ions of any given mass to charge ratio are trapped can be determined from the curvature C(m) given in equation <NUM> above, such that: <MAT>.

<FIG> shows this spatial width Δz(m) as a function of the mass to charge ratio of the ions.

<FIG> shows the mass to charge ratios of the ions in the ion guide as a function of the electrode number in the ion guide forming the ion trap, i.e. effectively as a function of the distance z along the ion trap. It can be seen that the mass to charge ratios of the ions trapped in the ion trap increase along the length of the ion trap. It can therefore be seen that ions of different mass to charge ratios can be ejected from the ion trap by ejecting ions from different regions of the length of the ion trap.

<FIG> shows the range of mass to charge ratios that are nominally trapped adjacent each electrode in the ion trap, as a function of the electrode number in the ion trap, i.e. effectively as a function of the distance z along the ion trap. This shows a decreasing mass range with increasing distance z from the end of ion trap, with a maximum range of approximately <NUM> Da.

The above example uses the DC and RF voltage profiles set out in equations <NUM> and <NUM> in order to generate the illustrated mass to charge ratio profile along the ion trap. However, different, choices of DC and/or RF voltage profiles may be used to tailor the mass to charge ratio distribution along the ion trap. Also, the ions may be separated within the ion trap such that they are arranged in order of increasing or decreasing mass to charge ratio by altering the arrangement of the DC and RF voltages applied the ion trap.

<FIG> shows a schematic of an arrangement that does not have all of the features of the independent claims and that may be used as a high pass mass to charge ratio filter, mimicking a low mass to charge ratio cut-off device. The system comprises a source of ions <NUM> (e.g. electrospray, REIMS, DESI, etc.), an ion trap or ion accumulation device <NUM> (e.g. SRIG trap), an ion guide filter <NUM> comprising an ion trap for separating the ions according to mass to charge ratio (e.g., as described above), an ion neutralising/destroying device <NUM> (e.g. pDRE lens), and onward transmission ion optics or a mass analyser <NUM>. Device <NUM> may be a mass to charge ratio analyser, such as Time of Flight (ToF) mass analyser or Orbitrap (RTM) etc. Alternatively, device <NUM> may be a gas filled ion guide that converts the pulsed beam received therein into a pseudo-continuous ion beam.

In use, ions from ion source <NUM> are accumulated in the ion trap <NUM> and are then pulsed into the ion filter <NUM>. The ion filter <NUM> comprises an ion trap of the type described above for separating the ions. Opposing forces are applied to the ions in the ion trap so as to cause them to separate within the filter <NUM> according to mass to charge ratio, as described above. The ions are allowed a short period of time after being pulsed into the filter <NUM> (typically a few milliseconds to a few tens of milliseconds) to cool, spatially separate and take up their equilibrium spatial positions. Ions having different mass to charge ratios become arranged at different positions within the filter <NUM>. For example, the ion distribution may be the same as that shown in <FIG>. In this arrangement the ions are arranged in order of mass to charge ratio within the filter <NUM>, with the lower mass ions arranged towards the exit of the filter <NUM>. The instrument acts as a high pass device and it is therefore desired to discard ions below a threshold mass to charge ratio. In order to do this, a controller and associated circuitry controls a voltage supply so as to apply a DC voltage to the ion trap of the filter <NUM> that travels along the portion of the filter <NUM> in which the unwanted ions are stored so as to force these ions out of the filter <NUM>.

The unwanted ions are swept out of the filter <NUM> and into the ion neutralising/destroying device <NUM>, which at this point is activate and neutralises or destroys the unwanted ions. The ion neutralising/destroying device <NUM> may be adapted and configured to electronically neutralise the ions. For example, the ion neutralising/destroying device <NUM> may comprise a controller and associated electronic circuitry that control a voltage supply to apply a voltage to an electrode that causes the unwanted ions to be deflected onto a surface that electrically neutralises them, e.g., so that they cannot be analysed by a downstream ion analyser. For example, the ion neutralising/destroying device <NUM> may deflect the ion onto an electrode that electrically neutralises the ions. Alternatively, the ion neutralising/destroying device <NUM> may react the ions with ions of opposite polarity so as to neutralise them. The neutralising device <NUM> is then deactivated and the remaining, desired ions are swept out of the filter <NUM> by travelling a DC voltage along the filter <NUM>. As the ion neutralising/destroying device <NUM> has been deactivated, the desired ions are transmitted therethrough to the device <NUM>.

The ion neutralising/destroying device <NUM> may alternatively be replaced with a device that simply discards the ions. For example, a device comprising a controller and associated electronic circuitry that control a voltage supply to apply a voltage to an electrode that causes the unwanted ions to ejected from the instrument, e.g., so that they cannot be analysed by a downstream ion analyser, may be used.

As an alternative to separating and arranging the ions in the filter <NUM> in the above manner, the ions could be separated in the filter <NUM> such that the higher mass to charge ratio ions are arranged towards the exit of the filter <NUM>. As such, a DC voltage may be travelled along the portion of the filter <NUM> in which the desired ions are stored so as to force these ions out of the filter <NUM>. These desired ions may then be onwardly transmitted to device <NUM>. Ions in the filter <NUM> having masses below the threshold value may be discarded, e.g. by subsequently transmitting them to the ion neutralising/destroying device <NUM> or ejecting them from the instrument in the manners described above. For example, the controller may switch off the trapping voltages in the filter <NUM> such that these unwanted ions are no longer trapped.

The instrument may alternatively be configured as a low pass filter. For example, the ions could be separated so as to be arranged in order of mass to charge ratio within the ion filter, with the lower mass ions arranged towards the exit of the filter <NUM>. However, this arrangement is a low pass filter and so only ions below a threshold mass to charge ratio are desired. As such, a DC voltage may be travelled along the portion of the mass filter in which the desired ions are stored so as to force these ions out of the filter <NUM>. These desired ions may then be onwardly transmitted to device <NUM>. Ions in the filter having masses above the threshold value may be neutralised or discarded, for example, in the manners described above.

Alternatively, the ions could be separated so as to be arranged in order of mass to charge ratio within the ion filter, with the higher mass ions arranged towards the exit of the filter <NUM>. In this arrangement, the a DC voltage is travelled along the portion of the mass filter <NUM> in which the unwanted ions are stored so as to force these ions out of the filter <NUM>. These unwanted ions are neutralised or discarded, e.g. in the manners described above. The desired ions may subsequently be swept out of the filter <NUM> by a travelling DC potential and onwardly transmitted to device <NUM>.

Alternatively, the device may be operated as a band pass filter. In this arrangement the ions are separated in the filter <NUM> in the same manner as described above. It is desired to neutralise or discard ions below a first threshold mass to charge ratio and to neutralise or discard ions above a second threshold value. If the ions are arranged in order of mass such that the low mass to charge ratios are arranged toward the exit of the filter <NUM>, then a DC voltage is travelled along the portion of the filter <NUM> in which the ions having masses below the first threshold are stored so as to force these ions out of the filter <NUM>. These ions are then neutralised or discarded, e.g. in the manners described above. A DC voltage is then travelled along the portion of the filter <NUM> in which the desired ions are stored, i.e. the ions having masses between the first and second threshold values. These desired ions are swept out of the filter <NUM> and are onwardly transmitted to device <NUM>. Ions in the filter <NUM> having masses above the second threshold value may then be neutralised or discarded, e.g. in the manners described above.

Alternatively, the ions could be arranged in order of mass to charge ratio within the ion filter, with the higher mass ions arranged towards the exit of the filter <NUM>. In this arrangement, a DC voltage is travelled along the portion of the filter <NUM> in which the ions having masses above the second threshold are stored so as to force these ions out of the filter <NUM>. These unwanted ions are neutralised or discarded, e.g. in the manners described above. A DC voltage is then travelled along the portion of the filter <NUM> in which the desired ions are stored, i.e. the ions having masses between the first and second threshold values. These desired ions are swept out of the filter <NUM> and are onwardly transmitted to device <NUM>. Ions in the filter <NUM> having mass to charge ratios below the first threshold value may then be neutralised or discarded, e.g. in the manners described above.

<FIG> shows a schematic of an instrument that does not have all of the features of the independent claims and that is the same as that shown in <FIG>, except wherein ions are orthogonally transferred from the ion filter <NUM> into an adjacent device <NUM>, rather than being further transmitted along the longitudinal axis of the instrument. As such, the ion neutralising/destroying device <NUM> may be omitted and replaced by a device <NUM> that has a controller and associated circuitry for controlling a voltage supply to apply voltages to the ion trap so as to orthogonally eject ions from the filter <NUM>. The device <NUM> may be, for example, an ion guide (such as a Stepwave (RTM) ion guide) that is conjoined with filter <NUM> so that ions travelling along the longitudinal axis of filter <NUM> may be selectively radially ejected into device <NUM> so as to travel along the longitudinal axis of the device <NUM>.

The instrument may be operated in any of the modes described above in relation to <FIG>, except that when the ions have been separated along the length of the filter <NUM> the desired ions may be orthogonally ejected from the filter <NUM> into the ion guide <NUM>. This is in contrast to the arrangement of <FIG>, wherein the desired ions are swept out of the filter <NUM> along its longitudinal axis. According to the instrument illustrated in <FIG>, the ions received in device <NUM> may be onwardly transmitted to device <NUM>.

Alternatively, rather than transferring desired ions into device <NUM>, only unwanted ions may be transferred into the adjacent device <NUM>. The desired ions may then be transferred along the longitudinal axis of filter <NUM> to an ion analyser.

The instrument may be operated both in simple filter modes in which the instrument may be operated in either low pass, high pass or band pass modes. Alternatively, the instrument may be operated in complex filter modes. For example, the instrument may be operated multi-pass filter modes in which ions are first trapped, separated and filtered according to a low pass, high pass or band pass mode in filter <NUM>; and at least some of the desired ions transmitted by the filter <NUM> are subsequently reintroduced into the filter <NUM> and are trapped, separated and filtered again according to a low pass, high pass or band pass mode.

It is contemplated that the desired ions may be transmitted in a mass to charge ratio dependent manner to a downstream device whose operation is scanned with time. For example, the scanned device may be a resolving quadrupole or other multipole in which the mass to charge ratios transmitted by the quadrupole or multipole is scanned with time. This coupling serves to increase the duty cycle of the scanned device.

Alternatively the separated ions may be fragmented or reacted in an active collision cell and, for example, a SWATH type experiment may be conducted. For example, ions having selected mass to charge ratio ranges may be transmitted as separate pulses from the filter <NUM> into an active collision, fragmentation or reaction cell, where the pulse shape or separation is maintained. The collision energy or the fragmentation or reaction rate may be alternated or switched between a high collision, fragmentation or reaction value in which substantial fragmentation or reaction of the ions is performed and a low collision, fragmentation or reaction value in which substantial fragmentation or reaction of the ions is not performed. The precursor ions from the first of the modes may be mass and/or ion mobility analysed and the fragment or product ions from the second of the modes may be mass and/or ion mobility analysed. The fragment or product ions may be assigned to their respective precursor ions, e.g., based on the times that they are mass and/or ion mobility analysed or based on their ion signal intensity profile shapes.

A second set of arrangements that do not have all of the features of the independent claims will now be described, in which the ion trap is used to separate ions and then eject the separated ions into an ion mobility separator (IMS) in a single pulse.

<FIG> shows a schematic arrangement of part of a prior art ion mobility spectrometer. The spectrometer comprises an ion trap <NUM> arranged upstream of an IMS device <NUM>. Ions are trapped in the ion trap <NUM> prior to being pulsed into the IMS device <NUM>. Prior to injection into the IMS device <NUM>, the ions are distributed substantially throughout the entire length of the ion trapping device <NUM> so as to maximise the ion storage capacity.

Rokushika et al (<NPL>) showed that the resolution of an IMS device is dependent upon the temporal width of the ion injection pulse into the device and the diffusion broadening that occurs along the drift path within the IMS device. The resolution of an IMS device can be described the following equation: <MAT> where t is the drift time of the ion along the drift path, W<NUM> is the initial ion pulse width, and Wd is the diffusion broadened peak width.

The diffusion broadened peak width Wd is given by: <MAT> where k is the Boltzmann constant, T is temperature, t is the drift time of the ion along the drift path, q is the electronic charge, E is the electric field in the drift region, and L is the length of the drift region.

The prior art arrangement of providing an ion trap device <NUM> upstream of the IMS device <NUM> is advantageous in that it increases the ion population that can be injected into the IMS device <NUM> at any one time. However, prior to injection, ions of any given mass to charge ratio are distributed throughout the ion trap <NUM> and so the initial ion pulse width W<NUM> for ions of any given mass is relatively wide, resulting in a relatively low resolution for ion mobility measurement when the ions are pulsed into the IMS device.

The second set of arrangements provide an improvement in measured ion mobility resolution through a reduction of the magnitude of W<NUM> for any given type of ion.

<FIG> shows a schematic arrangement of part of an ion mobility spectrometer according to the second set of arrangements. The instrument is the same as that in <FIG>, except that it is configured to spatially separate the ions in the ion trap <NUM> according to their mass to charge ratio. In the illustrated example, ions of a first mass are separated to one end of the ion trap <NUM> and ions of another mass are separated towards the other end of the ion trap <NUM>. Although only two groups of ions <NUM>,<NUM> are shown, other groups of ions of different mass to charge ratios may be separated and stored in groups that are arranged between the two illustrated groups <NUM>,<NUM>.

As the ions are separated within the ion trap <NUM>, ions of any given mass to charge ratio become confined within a relatively small region within the ion trap <NUM>. As such, when the ions are injected into the IMS device <NUM>, the initial ion pulse width W<NUM> for ions of any given mass to chare ratio is relatively narrow, even though a relatively large ion trap <NUM> has been used. This enables a large population of ions to be injected into the IMS device <NUM> without degrading the resolution of the ion mobility spectrometer. The separated ions may be injected into the IMS device <NUM> together in the same pulse into the IMS device <NUM>. The injection may be performed in a manner that maintains the separation of the ions, at least to some degree, during the injection.

As described above, ions may be spatially separated in the ion trap <NUM> using a combination a pseudo-potential electric field and a DC electric field. As also described above, with optimisation of the DC potential parameters, d<NUM> and d<NUM>, and the RF potential parameters, p<NUM> and p<NUM>, it is possible to obtain reasonable voltage levels and good spatial separation of the ions within the ion trap. In the description below, optimisation of the parameters assumes an ion trap length of <NUM> and a distribution of ions in the trap for ions having a range of mass to charge ratios of <NUM> to <NUM> Da.

<FIG> shows the DC voltage potential profile Vdc(z) along the ion trap <NUM> achieved using values of d<NUM>= -<NUM>, d<NUM>= -<NUM>, a maximum Vdc = -<NUM> V, and ω = <NUM>.

<FIG> shows the RF voltage potential profile Vx(z) along the ion trap <NUM> achieved using parameters p<NUM> = -<NUM> and p<NUM> = -<NUM> and a maximum Vx = <NUM> V.

<FIG> shows a graph of the position z at which the total potential Vtot is minimum as a function of ion mass to charge ratio, for ions of mass to charge m between <NUM> and <NUM> Da, and for the combination voltage profiles shown in <FIG>.

The ions are cooled by the buffer or background gas in the ion trap <NUM> and they reach thermal energy. A worst case assumption would be that the residual axial energy ΔV of the ions was ten times this value, say approximately ΔV= <NUM> eV. This assumption then allows the spatial width Δz(m) along the z-direction of the ion trap that any given ion will reside within to be determined from equation <NUM> above, i.e. +/-<NUM> V from the central potential position.

Once the ions have been separated in the ion trap <NUM>, the separated ions are injected into the IMS device <NUM>. This may be performed by travelling a voltage along the ion trap <NUM>. For example, a controller and associated circuitry may control a voltage supply so as to apply one or more voltage (e.g., a DC voltage) to the ion trap <NUM> that travels along the ion trap <NUM> so as to pulse ions from the ion trap <NUM> into the IMS device <NUM>. The velocity v of the ions exiting the ion trap <NUM> may be controlled, e.g., by setting or controlling the velocity of the travelling voltage. For example, the velocity v is typically set to the order of <NUM>/s. Therefore, the spatial spread Δz of ions having any given mass to charge ratio may be mapped into a temporal spread Δt of these ions leaving the ion trap <NUM>, wherein Δt = Δz/v.

<FIG> shows a plot of the temporal spread of the ions Δt as a function of mass to charge ratios of the ions.

The drift time t in equation <NUM> above is dependent upon the mass to charge ratio of the ions. The drift time t(m) may be calculated using the following equation: <MAT> where Ld is the length of the ion mobility drift tube, Ed is the electric field along the drift tube, p is the pressure, mb is the molecular mass of the buffer gas, and Ω (m) is the collision cross-sectional area. For simplicity, only ions of single charge have been considered here.

The collision cross-sectional area Ω (m) may be estimated by the following equation, which is based upon the molecular radii of the ion and buffer gas molecules: <MAT>.

<FIG> shows a plot of drift time Dt as a function of mass to charge ratio. This plot was obtained using the equation for t(m) above and substituting reasonable values for the operational parameters, which were an electric field along the drift tube Ed of <NUM> kV/m, a length of the ion mobility drift tube Ld of <NUM>, a temperature T of <NUM>, and a pressure p of <NUM> mbar nitrogen.

The parameter Δt is equivalent to the initial ion pulse width Wo in equation <NUM> above. The diffusion broadened peak width Wd may be calculated using the estimated drift times t(m) from equation <NUM> above. Accordingly, the resolution R may be determined from equation <NUM> above.

<FIG> shows two plots of resolution R against mass to charge ratio of the ions. The lower plot corresponds to that of a prior art technique that does not spatially separate the ions in the ion trap <NUM> (i.e. using the instrument shown in <FIG>) and which gates ions into the IMS device <NUM> using a gate time of <NUM>. In other words, the initial ion pulse width Wo is <NUM>. The upper plot corresponds to the second set of arrangements that spatially separates the ions in the ion trap <NUM>. <FIG> indicates that the second set of arrangements provide a significant increase in the resolution of the ion mobility spectrometer over the prior art spectrometer. The enhancement in resolution increases with decreasing ion mobility drift time. For mass to charge ratios up to <NUM> Da, there is a greater than two fold enhancement in resolution. The second set of arrangements allow ion mobility measurements to be made with high resolution, even though a large ion trap <NUM> is utilised to inject a large ion population into the IMS device <NUM> at any one time.

The second set of arrangements introduce a mass to charge ratio dependent shift in the measured drift time, since ions of different mass to charge ratios are separated and stored in the ion trap <NUM> at different distances from the entrance to the IMS device <NUM>. However, this may be easily taken care of by calibration. In addition, the pre-separation may be ion mobility dependent and may result in an increase in temporal separation.

The IMS device <NUM> may comprise a drift length having a static DC field arranged across it for forcing ions to separate within the IMS device <NUM> according to ion mobility. Alternatively, an electric potential barrier may be travelled along the drift length of the IMS device <NUM> in order to force the ions to separate according to ion mobility in the IMS device <NUM>.

Embodiments of the present invention will now be described, in which the ion trap is used to separate ions and then eject separated groups of ions into a discontinuous ion analyser at different times.

<FIG> shows a schematic of part of a conventional Time of Flight (ToF) mass spectrometer. The apparatus comprises an ion trap <NUM> of length Z, an ion transfer region <NUM> of length L, and a pusher region <NUM> of an orthogonal acceleration time of flight (oa-ToF) mass analyser having a length ΔL.

In use, ions are trapped in the ion trap <NUM> and are pulsed into the ion transfer region <NUM>. Ion optics in the transfer region <NUM> guide the ions to the pusher region <NUM>. The pusher region <NUM> pulses an orthogonal acceleration electric field such that the ions are accelerated orthogonally from their flight path and into the time of flight region of the ToF mass analyser. In order to achieve the optimum duty cycle of the oa-ToF spectrometer, all of the ions released from the trap <NUM> must be spatially located within the pusher region <NUM> when the orthogonal acceleration field is applied. The following calculations can be made to determine the mass to charge ratios of the ions that would fulfil this condition.

The time of flight T<NUM> for an ion of mass to charge ratio m<NUM> to travel from the exit of the ion trap <NUM> (at z=<NUM>) to the end of the pusher region <NUM> is as follows: <MAT> where M is the atomic mass unit, q is the electronic charge constant, Vz is the potential that the ion experiences on its journey through the ion transfer optics in the transfer region <NUM>, and (L+ΔL) is the distance from the exit of the ion trapping region <NUM> to the end of the pusher region <NUM>.

The time of flight T<NUM> of a second ion of higher mass to charge ratio m<NUM> to travel the distance L from the exit of the ion trapping region <NUM> (at z=<NUM>) to the entrance of the pusher region <NUM> is as follows: <MAT>.

By setting time of flight T<NUM> to be equal to the time of flight T<NUM> one can determine the mass to charge ratio m<NUM> of the ions that have reached the entrance to the pusher region <NUM> at the same time that ions of mass to charge ratio m<NUM> have reached the exit of the pusher region <NUM>. This results in the following equation: <MAT>.

In order to increase the duty cycle of the ToF mass analyser it is required that the pusher is presented with a restricted range of mass to charge ratios, otherwise all of the ions will not be located within the pusher region <NUM> at the time that the orthogonal acceleration extraction pulse is applied. The required range of mass to charge ratios mi, mi-<NUM> as a function of the sequential push number i, is as follows: <MAT>.

<FIG> shows the values of mi as a function of the pulse number i for an instrument having a typical ion transfer region <NUM> length L and a typical pusher region <NUM> length ΔL. In this example the ion transfer region length L is <NUM>, the pusher region length ΔL is <NUM>, and the range of mass to charge ratios pulsed in the first pulse is m<NUM> = <NUM> Da.

The present invention provides an improvement over such conventional discontinuous ion analysers by spatially separating the ions according to a physicochemical property (e.g., mass to charge ratio) in an ion trap upstream of the discontinuous ion analyser.

As described above, according to the embodiments of the present invention, ions may be spatially separated in the ion trap using a combination a pseudo-potential electric field and a DC electric field so as to provide the relationship in equation <NUM> above, from which can be determined the position z at which the pseudo-potential minimum for any given ion is located, and hence the position at which that ion will remain trapped.

As the ions are separated along the ion trap according to mass to charge ratio, ions may be swept out of the ion trap from different positions within the ion trap in order to eject different ranges of mass to charge ratio into the downstream ion analyser. In order to do this, a controller and associated circuitry may control a voltage supply so as to apply a DC voltage to the ion trap that travels along the ion trap so as to eject the ions into the downstream ion analyser.

Substituting mi from equation <NUM> above into equation <NUM>, gives the distance along the ion trap that must be swept out by the travelling voltage in the ith pulse. This distance zi is given by the following equation: <MAT>.

As described above, with optimisation of the DC potential parameters, d<NUM> and d<NUM>, and the RF potential parameters, p<NUM> and p<NUM>, it is possible to obtain reasonable voltage levels and good spatial separation of the ions within the ion trap.

<FIG> shows the position zi along the ion trap from which the travelling voltage sweeps ions towards the exit of the ion trap (wherein the exit is at z = <NUM>) as a function of push number i, for pushes i between i = <NUM> and i = <NUM>. In this model, the length of the ion trapping device is <NUM> and ω = <NUM>. Optimised values for the DC voltage gave d<NUM> = - <NUM> and d<NUM> = -<NUM>, with a maximum of -<NUM> V and the RF voltage p<NUM>= -<NUM> and p<NUM>= <NUM> and shows a maximum of approximately <NUM> V.

As can be seen from <FIG>, the distance that the travelling voltage must travel along the ion trap increases in subsequent push numbers. This enables ions from different depths within the ion trap to be received in the pusher region <NUM> of the ToF mass analyser when different orthogonal acceleration pulses are applied. As ions having different ranges of mass to charge ratio are trapped at different depths in the ion trap (i.e. different values of z), ions having different ranges of mass to charge ratio are analysed in the different orthogonal acceleration pulses.

<FIG> shows the length Δz of the ion trap that both contains trapped ions and from which ion are extracted, as a function of the ToF push number i. It can be seen that the ions trapped over a small length (e.g. <NUM>) of the ion trap are swept into the pusher region for the first push at i = <NUM>. The next sweep extracts ions trapped over a larger length of the ion trap, such that these ions are swept into the pusher region for the second push at i = <NUM>. It will be seen that subsequent sweeps extract ions that were trapped over progressively increasing lengths of the ions trap. <FIG> shows data that would cover a mass range between <NUM> and approximately <NUM> Da, requiring a minimum sweep of approximately <NUM> of ion guide and thus is entirely possible with current technologies.

The embodiments of the invention enables ions having a relatively large range of mass to charge ratios to be trapped in the ion trap <NUM>, without the ions being ejected from the ion trap <NUM> and into the pusher region <NUM> in a manner that overfills the pusher region <NUM> at the time the orthogonal acceleration extraction pulse is applied. By spatially separating the ions within the ion trap, ions of any given range of mass to charge ratios become confined within a sub-region (which may be a relatively small region) of the ion trap. Different ranges of mass to charge ratios may then be swept out of the ion trap and into the mass analyser at different times by ejecting ions from different regions of the ion trap at different times.

<FIG> shows an embodiment of the ion trap <NUM> that may be used in the various embodiments described herein. The ion trap <NUM> may be a linear ion trap and comprises a plurality of apertured electrodes <NUM>. An AC or RF voltage supply <NUM> may apply AC or RF voltages to the electrodes <NUM> so as to radially confine ions within the ion trap <NUM>. Opposite phases of an AC or RF voltage may be applied to axially adjacent electrodes. Different AC or RF voltages (e.g., different magnitudes) may be applied to different electrodes <NUM> along the ion trap <NUM> so as to generate a first force on the ions in a first direction along the axial length of the ion trap <NUM>. A DC voltage supply <NUM> may apply DC voltages to the electrodes <NUM>. Different DC voltages (e.g., different magnitudes) may be applied to different electrodes <NUM> along the ion trap <NUM> so as to generate a second force on the ions in a second direction along the axial length of the ion trap <NUM>, opposite to the first direction. Additionally, or alternatively, a pump <NUM> may be provided to generate a gas flow through the ion trap <NUM> that generates a force on the ions in the second direction.

A controller <NUM> is provided that comprises an ion separator. The controller and ion separator contain a processor and electronic circuitry that are configured to control the voltage supplies <NUM>,<NUM> (and/or pump <NUM>) so as to apply the voltages to the electrodes <NUM> (and/or pump the gas through the ion trap <NUM>) that cause the first and second forces to be generated on the ions. This causes the ions to separate along the axial length of the ion trap <NUM> according to mass to charge ratio, as described above.

The controller <NUM> also comprises an ion driving or pulsing circuit that contain a processor and electronic circuitry configured to control the voltage supplies <NUM>,<NUM> (and/or pump <NUM>) so as to apply voltages to the electrodes <NUM> (and/or control the gas supply) to cause ions to be driven or pulsed out of the ion trap, after they have been separated.

Although the present invention has been described with reference to various embodiments, it will be understood by those skilled in the art that various changes in form and detail may be made without departing from the scope of the invention as set forth in the accompanying claims.

For example, although a stacked ring ion guide has been described as being used in the ion trap, other geometries of electrodes may be used.

Although a travelling wave has been described as the means by which ions are extracted from the trap, alternative methods of releasing the ions from the ion trap in a controlled manner may be used. For example, the axial DC potential or pseudo-potential gradient may be ramped so as to force ions out of the ion trap, or may be altered along different lengths of the ion trap at different times so as to eject ions.

Although the spatial separation has been described as being achieved by using opposing forces on the ions generated by pseudo-potential and an opposing DC potential, the spatial separation may be achieved by other methods. For example, one of the opposing forces may be applied from a gas flow instead of the DC potential or pseudo-potential gradient.

Although various values of the RF and DC voltages have been described herein, these parameters and other operational parameters of the ion trap may be varied according to the desired mode of operation and/or the ions trapped therein.

The ions may be caused to separate in the ion trap by ion mobility instead of mass to charge ratio, or by a combination of mass to charge ratio and ion mobility.

Claim 1:
A method of mass spectrometry and/or ion mobility spectrometry comprising:
trapping ions in an ion trap (<NUM>, <NUM>); and then
spatially separating the ions within the ion trap according to at least one physicochemical property so that ions having different values of said physicochemical property are trapped in different regions of the ion trap; wherein said step of spatially separating the ions comprises applying a first force on the ions within the ion trap in a first direction, said force having a magnitude that is dependent upon the value of said at least one physicochemical property of the ions, and applying a second force on these ions in the opposite direction, and wherein said first and second forces are counterbalanced at different locations within the ion trap for ions having different physicochemical property values, such that different ions are trapped at said different regions; and then
driving or pulsing first trapped ions out of a first region of the ion trap and into a discontinuous ion analyser at a first time, whilst retaining other ions trapped in the ion trap;
analysing said first ions in a first cycle of said discontinuous ion analyser;
driving or pulsing second trapped ions out of a second, different region of the ion trap and into the discontinuous ion analyser at a second, subsequent time; and
analysing said second ions in a different cycle of said discontinuous ion analyser.