ACCELERATOR FOR MULTI-PASS MASS SPECTROMETERS

Abstract

Improved pulsed ion sources and pulsed converters are proposed for multi-pass time-of-flight mass spectrometer, either multi-reflecting (MR) or multi-turn (MT) TOF. A wedge electrostatic field 45 is arranged within a region of small ion energy for electronically controlled tilting of ion packets 54 time front. Tilt angle γ of time front 54 is strongly amplified by a post-acceleration in a flat field 48. Electrostatic deflector 30 downstream of the post-acceleration 48 allows denser folding of ion trajectories, whereas the injection mechanism allows for electronically adjustable mutual compensation of the time front tilt angle, i.e. γ=0 for ion packet in location 55, for curvature of ion packets, and for the angular energy dispersion. The arrangement helps bypassing accelerator 40 rims, adjusting ion packets inclination angles α2, and what is most important, compensating for mechanical misalignments of the optical components.

Description

FIELD OF INVENTION

The invention relates to the area of time of flight mass spectrometers, multi-turn and multi-reflecting time-of-flight mass spectrometers with pulsed ion sources and pulsed converters, and is particularly concerned with improved ion injection.

BACKGROUND

Time-of-flight mass spectrometers (TOF MS) are widely used for combination of sensitivity and speed, and lately with the introduction of ion mirrors and multi-reflecting schemes, for their high resolution and mass accuracy. Pulsed sources are used for intrinsically pulsed ionization methods, such as Matrix Assisted Laser Desorption and Ionization (MALDI), Secondary Ionization (SIMS), and pulsed EI. The first two ion sources become more and more popular for mass spectral surface imaging, where a relatively large surface area is analyzed simultaneously while using mapping properties of TOF MS.

Even more popular are TOF MS, where pulsed converters are used to form pulsed ion packets out of continuous ion beams produced by ion sources like Electron Impact (EI), Electrospray (ESI), Atmospheric pressure ionization (APPI), atmospheric Pressure Chemical Ionization (APCI), Inductively couple Plasma (ICP) and gaseous (MALDI). Most common pulsed converters are orthogonal accelerators (WO9103071) and radiofrequency ion traps with pulsed radial ejection, lately used for ion injection into Orbitraps (RTM). Two aspects of prior art are relevant to the present invention: (a) all ion sources and converters for TOF MS employ pulsed accelerating fields; (b) a significant portion of ion sources and converters are spatially wide, so that bypassing of ion sources and converters by ion packets returned after one pass (reflection or turn) becomes an issue.

The resolution of TOF MS has been substantially improved in multi-pass TOFMS (MPTOF), by reflecting ions multiple times between ion mirrors in multi-reflecting TOF (MRTOF) mass analysers [e.g. as described in SU1725289, U.S. Pat. Nos. 6,107,625, 6,570,152, GB2403063, U.S. Pat. No. 6,717,132, incorporated herein by reference], or by turning ions multiple times in electrostatic sectors in multi-turn TOF (MTTOF) mass analysers [e.g. as described in U.S. Pat. Nos. 7,504,620, 7,755,036, and M. Toyoda, et. al, J. Mass Spectrom. 38 (2003) 1125, incorporated herein by reference].

MPTOF analyzers are arranged to fold ion trajectories for substantial extension of the ion flight path (e.g. 10-50 m or more) within commercially reasonably sized (0.5-1 m) instruments. The ion path folding in MRTOF analysers is arranged with ion packet reflection in the X-direction combined with slow ion drift in the drift Z-direction, thus producing zigzag ion trajectories. The ion path folding in MTTOF is arranged with ion circular, oval or figure-of-eight loops in the X-Y plane combined with slow drift in the drift Z-direction, thus producing spiral ion motion. The term “pass” generalizes ion mirror reflections and ion turns. The resolving power (also referred as resolution) of MP-TOF analysers grows at larger number of passes N by reducing the effect of the initial time spread of ion packets and of the detector time spread.

Most MPTOF analysers employ two dimensional (2D) electrostatic fields in the XY-plane between electrodes, substantially elongated in the drift Z-direction. The 2D-fields of ion mirrors or sectors are carefully engineered to provide for isochronous ion motion and for spatial ion packet confinement in the XY-plane. By nature, the electrostatic 2D-fields have zero component E_Z=0 in the orthogonal drift Z-direction, i.e. they have no effect on the ion packets free propagation and its expansion in the drift Z-direction.

In earlier MPTOF schemes, the control over ion motion in the drift direction was arranged by the ion injecting mechanisms in ion sources or ion pulsed converters, defining the inclination angle of ion trajectory in the analyzer. In an attempt to increase MPTOF resolution by using denser folding of the ion trajectory, the injection angle α (to axis X) of ion packets shall be reduced, thus, requiring much lower energies of the injected continuous ion beam. Lower injection energies affect the ion beam admission into the OA and increase the ion packet angular divergence Δα. Ions start hitting rims of the accelerator and ion detector, and may produce trajectories that overlap, thus confusing spectra.

To address those problems, multiple complex solutions have been proposed to define the ion drift advance per reflection, to prevent or compensate the angular divergence of ion packets, and to withstand various distortions, such as stray fields and mechanical distortions of analyzer electrodes: e.g. U.S. Pat. No. 7,385,187 proposed periodic lens and edge deflectors for MRTOF analysers; U.S. Pat. No. 7,504,620 proposed laminated sectors for MTTOF analysers; WO2010008386 and then US2011168880 proposed quasi-planar ion mirrors having weak (but sufficient) spatial modulation of mirror fields; U.S. Pat. No. 7,982,184 proposed splitting mirror electrodes into multiple segments for arranging E_Z field; U.S. Pat. No. 8,237,111 and GB2485825 proposed electrostatic traps with three-dimensional fields, though without sufficient isochronicity in all three dimensions and without non-distorted regions for ion injection; WO2011086430 proposed first order isochronous Z-edge reflections by tilting ion mirror edge combined with reflector fields; U.S. Pat. No. 9,136,101 proposed bent ion MRTOF ion mirrors with isochronicity recovered by trans-axial lens. Though prior art solutions do solve the problem of controlling Z-motion, they have several drawbacks, comprising: (i) technical complexity; (ii) additional time aberrations, affecting resolution; (iii) limited length of ion packets and limited duty cycle and charge capacity of pulsed converters; and (iv) fixed arrangement with low tolerance to manufacturing faults. Those drawbacks become particularly problematic when trying to construct a compact and low cost MPTOF instrument for higher resolutions.

SUMMARY

From a first aspect the present invention provides a pulsed ion accelerator for a mass spectrometer comprising: a plurality of electrodes and at least one voltage supply arranged and configured to generate a wedge-shaped electric field region; wherein the ion accelerator is configured to apply a pulsed voltage to at least one of said electrodes for pulsing ions out of the ion accelerator, wherein the ions have a time front arranged in a first plane at the time the pulsed voltage is initiated, and wherein the ion accelerator is configured such that the pulsed ions pass through the wedge-shaped electric field region so as to cause the time front of the ions to be tilted at an angle to the first plane.

The above pulsed ion accelerator tilts the time front of the ions it pulses out. By introducing such a tilted time front, the pulsed ion accelerator is able to compensate for time front tilting that may occur at ion optical components of the mass spectrometer that are downstream of the pulsed ion accelerator. The embodiments are also able to introduce a relatively large time front tilt whilst altering the mean ion trajectory by only a relatively small angle.

For the avoidance of doubt, the time front of the ions may be considered to be a leading edge/area of ions in the ion packet having the same mass to charge ratio (and which may have the mean average energy).

The pulsed ion accelerator is an orthogonal accelerator.

The pulsed ion accelerator may be arranged to receive ions along a first axis and pulse the ions substantially orthogonally to the first axis.

The pulsed ion accelerator may comprise electrodes arranged and configured for generating said wedge-shaped electric field region therebetween such that equipotential field lines in the wedge-shaped electric field region are angled to each other so as to form the wedge-shape.

Therefore, the equipotential field lines may converge towards one another in a direction towards a first end of the wedge-shaped electric field region, and diverge away from one another in a direction towards a second opposite end of the wedge-shaped electric field region.

The first and second ends may be spaced apart in a direction substantially along said first axis along which ions are received.

Ions travelling through the wedge-shaped electric field region may be accelerated by the wedge-shaped electric field by an amount that increases as a function of distance towards the first end, since the equipotential field lines converge towards the first end. This may cause the time front of the ions to be tilted.

The pulsed ion accelerator may comprise one or more first electrode arranged in a first plane and one or more second electrode arranged in a second plane that is angled to the first plane so as to define the wedge-shaped electric field region between the one or more first electrode and one or more second electrode.

The pulsed ion accelerator may comprise one or more first electrode arranged in a first plane and a plurality of second electrodes arranged in a second plane, wherein the ion accelerator is configured to apply different voltages to different ones of the second electrodes so as to define the wedge-shaped electric field region between the one or more first electrode and the second electrodes.

This enables the time front tilt angle to easily be varied by varying the potentials applied to the second electrodes.

The first and second plane may be parallel.

The second electrodes may be connected by a resistive chain such that a voltage supply connected to the resistive chain applies different electrical potentials to the second electrodes.

The plurality of second electrodes may be arranged on a printed circuit board (PCB).

The one or more first electrodes may be a plurality of first electrodes, and the ion accelerator may be configured to apply different voltages to the first electrodes so as to define the wedge-shaped electric field region. This enables the time front tilt angle to be varied by varying the potentials applied to the first electrodes. The first electrodes may be connected by a resistive chain such that a voltage supply connected to the resistive chain applies different electrical potentials to the first electrodes. The first electrodes may be arranged on a printed circuit board (PCB).

PCB as used herein may refer to a component containing conductive tracks, pads and other features etched from, printed on, or deposited on one or more sheet layers of material laminated onto and/or between sheet layers of a non-conductive substrate.

In embodiments in which electrodes are arranged on a PCB, a resistive layer may be provide between the electrodes, so as to avoid the insulating material of the substrate from becoming electrically charged.

Embodiments are also contemplated in which at least some of the electrodes connected by the resistive chain are replaced by a resistive layer.

The pulsed ion accelerator may comprise electrodes spaced apart in a dimension for defining the wedge-shaped electric field region therebetween, and the ion accelerator may be configured to pulse ions in said dimension.

The electrodes for generating said wedge-shaped electric field region may be arranged so that equipotential field lines of the wedge-shaped electric field extend substantially in a first direction and the ion accelerator is configured to pulse the ions through the wedge-shaped electric field substantially transverse to the equipotential field lines.

The ion accelerator may be arranged and configured to receive ions travelling substantially in the first direction.

The ion accelerator may be arranged to receive ions at the wedge-shaped electric field region.

The ion accelerator may be arranged and configured to receive ions travelling in a first direction along a first axis that is substantially parallel to equipotential field lines of the wedge-shaped electric field.

The equipotential field lines of the wedge-shaped electric field may diverge, or converge, as a function of distance in the first direction.

Alternatively, the ion accelerator may be arranged to receive ions at an ion receiving region and then pulse the ions downstream into the wedge-shaped electric field region of the ion accelerator.

The pulsed ion accelerator may be configured to pulse said wedge-shaped electric field for pulsing ions out of the ion accelerator.

The pulsed ion accelerator may comprise an ion acceleration region downstream of the wedge-shaped electric field region for amplifying the time front tilt introduced by the wedge-shaped electric field.

The pulsed ion accelerator may comprise a voltage supply and electrodes configured to apply a static electric field in the ion acceleration region for accelerating the ions; and/or a voltage supply and electrodes configured to apply an electric field in the ion acceleration region having parallel equipotential field lines for accelerating the ions.

The pulsed ions may travel through the ion acceleration region substantially orthogonal to the parallel equipotential field lines.

The pulsed ion accelerator may comprise an ion deflector located downstream of the pulsed ion accelerator and configured to deflect the average ion trajectory of the ions, thereby tilting the angle of the time front of the ions received by the ion deflector. The wedge-shaped electric field region of the pulsed ion accelerator may be configured to tilt the time front of the ions passing therethrough so as to at least partially counteract the tilting of the time front by the ion deflector.

The angle of the time front may therefore be moved at least partially back towards the first plane (i.e. the angle the time front was at when the pulsed voltage was initiated) when the ions exit the ion deflector.

The initial mean ion energy of the ions prior to acceleration in the pulsed ion accelerator may be (significantly) smaller than the mean ion energy of the ions within said ion deflector.

It has been recognised that a conventional ion deflector inherently has a relatively high focusing effect on the ions, hence undesirably increasing the angular spread of the ion trajectories exiting the deflector, as compared to the angular spread of the ion trajectories entering the ion deflector. This may cause excessive spatial defocusing of the ions downstream of the focal point, resulting in ion losses and/or causing ions to travel significantly different path lengths through the spectrometer before they reach the detector. The mass resolution of the spectrometer may be adversely affected. Embodiments of the present invention provide an ion deflector configured to generate a quadrupolar field that controls the spatial focusing of the ions, e.g. so as to maintain substantially the same angular spread of the ions passing therethrough, or to allow only the desired amount of spatial focusing of the ions.

The pulsed ion accelerator may be one of: (i) a MALDI source; (ii) a SIMS source; (iii) a mapping or imaging ion source; (iv) an electron impact ion source; (v) a pulsed converter for converting a continuous or pseudo-continuous ion beam into ion pulses; (vi) an orthogonal accelerator; (vii) a pass-through orthogonal accelerator having an electrostatic ion guide; or (viii) a radio-frequency ion trap with pulsed ion ejection.

The present invention also provides a mass spectrometer comprising: a multi-pass time-of-flight mass analyser or electrostatic ion trap having the pulsed ion accelerator as described hereinabove, and electrodes arranged and configured so as to provide an ion drift region that is elongated in a drift direction (z-dimension) and to reflect or turn ions multiple times in an oscillating dimension (x-dimension) that is orthogonal to the drift direction.

The multi-pass time-of-flight mass analyser may be a multi-reflecting time of flight mass analyser having two ion mirrors that are elongated in the drift direction (z-dimension) and configured to reflect ions multiple times in the oscillation dimension (x-dimension), wherein the pulsed ion accelerator is arranged to receive ions and accelerate them into one of the ion mirrors. Alternatively, the multi-pass time-of-flight mass analyser may be a multi-turn time of flight mass analyser having at least two electric sectors configured to turn ions multiple times in the oscillation dimension (x-dimension), wherein the pulsed ion accelerator is arranged to receive ions and accelerate them into one of the sectors.

Where the mass analyser is a multi-reflecting time of flight mass analyser, the mirrors may be gridless mirrors.

Each mirror may be elongated in the drift direction and may be parallel to the drift dimension.

It is alternatively contemplated that the multi-pass time-of-flight mass analyser or electrostatic trap may have one or more ion mirror and one or more sector arranged such that ions are reflected multiple times by the one or more ion mirror and turned multiple times by the one or more sector, in the oscillation dimension.

The spectrometer may comprise an ion deflector located downstream of said pulsed ion accelerator, and that is configured to back-steer the average ion trajectory of the ions, in the drift direction, thereby tilting the angle of the time front of the ions received by the ion deflector.

The average ion trajectory of the ions travelling through the ion deflector may have a major velocity component in the oscillation dimension (x-dimension) and a minor velocity component in the drift direction. The ion deflector back-steers the average ion trajectory of the ions passing therethrough by reducing the velocity component of the ions in the drift direction. The ions may therefore continue to travel in the same drift direction upon entering and leaving the ion deflector, but with the ions leaving the ion deflector having a reduced velocity in the drift direction. This enables the ions to oscillate a relatively high number of times in the oscillation dimension, for a given length in the drift direction, thus providing a relatively high resolution.

The wedge-shaped electric field region of the pulsed ion accelerator may be configured to tilt the time front of the ions passing therethrough so as to at least partially counteract the tilting of the time front by the ion deflector.

The angle of the time front may therefore be moved at least partially back towards the first plane (i.e. the angle the time front was at when the pulsed voltage was initiated) when the ions exit the ion deflector.

The ion deflector may be configured to generate a quadrupolar field for controlling the spatial focusing of the ions in the drift direction.

It has been recognised that a conventional ion deflector inherently has a relatively high focusing effect on the ions, hence undesirably increasing the angular spread of the ion trajectories exiting the deflector, as compared to the angular spread of the ion trajectories entering the ion deflector. This may cause excessive spatial defocusing of the ions downstream of the focal point, resulting in ion losses and/or causing ions to undergo different numbers of oscillations in the spectrometer before they reach the detector. This may cause spectral overlap due to ions from different ion packets being detected at the same time. The mass resolution of the spectrometer may also be adversely affected. Such conventional ion deflectors are therefore particularly problematic in multi-pass time-of-flight mass analysers or multi-pass electrostatic ion traps, since a large angular spread of the ions will cause any given ion packet to diverge a relatively large amount over the relatively long flight path through the device. Embodiments of the present invention provide an ion deflector configured to generate a quadrupolar field that controls the spatial focusing of the ions in the drift direction, e.g. so as to maintain substantially the same angular spread of the ions passing therethrough, or to allow only the desired amount of spatial focusing of the ions in the z-direction.

The quadrupolar field for in the drift direction may generate the opposite ion focusing or defocusing effect in the dimension orthogonal to the drift direction and oscillation dimension. However, it has been recognised that the focal properties of MPTOF mass analyser (e.g. MRTOF mirrors) or electrostatic trap are sufficient to compensate for this.

The ion deflector may be configured to generate a substantially quadratic potential profile in the drift direction.

The ion deflector may back steer all ions passing therethrough by the same angle; and/or the ion deflector may control the spatial focusing of the ion packet in the drift direction such that the ion packet has substantially the same size in the drift dimension when it reaches an ion detector in the spectrometer as it did when it enters the ion deflector.

The ion deflector may control the spatial focusing of the ion packet in the drift direction such that the ion packet has a smaller size in the drift dimension when it reaches a detector in the spectrometer than it did when it entered the ion deflector.

At least one voltage supply may be provided that is configured to apply one or more first voltage to one or more electrode of the ion deflector for performing said back-steer and one or more second voltage to one or more electrode of the ion deflector for generating said quadrupolar field for said spatial focusing, wherein the one or more first voltage is decoupled from the one or more second voltage.

The ion deflector may comprise at least one plate electrode arranged substantially in the plane defined by the oscillation dimension and the dimension orthogonal to both the oscillation dimension and the drift direction (X-Y plane), wherein the plate electrode is configured back-steer the ions; and the ion deflector may comprise side plate electrodes arranged substantially orthogonal to the at least one plate electrode and that are maintained at a different potential to the plate electrode for controlling the spatial focusing of the ions in the drift direction.

The side plates may be Matsuda plates.

The at least one plate electrode may comprise two electrodes and a voltage supply for applying a potential difference between the electrodes so as to back-steer the average ion trajectory of the ions, in the drift direction.

The two electrodes may be a pair of opposing electrodes that are spaced apart in the drift direction.

However, it is contemplated that only the upstream electrode (in the drift direction) may be provided, so as to avoid ions hitting the downstream electrode.

The ion deflector may be configured to provide said quadrupolar field by comprising one or more of: (i) a trans-axial lens/wedge; (iii) a deflector with aspect ratio between deflecting plates and side walls of less than 2; (iv) a gate shaped deflector; or (v) a toroidal deflector such as a toroidal sector.

The ion deflector may be arranged such that it receives ions that have already been reflected or turned in the oscillation dimension by the multi-pass time-of-flight mass analyser or electrostatic ion trap; optionally after the ions have been reflected or turned only a single time in the oscillation dimension by the multi-pass time-of-flight mass analyzer or electrostatic ion trap.

The location of the deflector directly after the first ion mirror reflection allows yet denser ray folding

The pulsed ion accelerator and ion deflector may tilt the time front so that it is aligned with the ion receiving surface of the ion detector and/or to be parallel to the drift direction (z-dimension).

The mass analyser or electrostatic trap may be an isochronous and/or gridless mass analyser or an electrostatic trap.

The mass analyser or electrostatic trap may be configured to form an electrostatic field in a plane defined by the oscillation dimension and the dimension orthogonal to both the oscillation dimension and drift direction (i.e. the XY-plane).

This two-dimensional field may have a zero or negligible electric field component in the drift direction (in the ion passage region). This two-dimensional field may provide isochronous repetitive multi-pass ion motion along a mean ion trajectory within the XY plane.

The energy of the ions received at the pulsed ion accelerator and the average back steering angle of the ion deflector may be configured so as to direct ions to an ion detector after a pre-selected number of ion passes (i.e. reflections or turns).

The spectrometer may comprise an ion source. The ion source may generate an substantially continuous ion beam or ion packets.

The pulsed ion accelerator may be a gridless orthogonal accelerator.

The pulsed ion accelerator has a region for receiving ions (a storage gap) and may be configured to pulse ions orthogonally to the direction along which it receives ions. The pulsed ion accelerator may receive a substantially continuous ion beam or packets of ions, and may pulse out ion packets.

The drift direction may be linear (i.e. a dimension) or it may be curved, e.g. to form a cylindrical or elliptical drift region.

The mass analyser or ion trap may have a dimension in the drift direction of: ≤1 m; ≤0.9 m; ≤0.8 m; ≤0.7 m; ≤0.6 m; or ≤0.5 m. The mass analyser or trap may have the same or smaller size in the oscillation dimension and/or the dimension orthogonal to the drift direction and oscillation dimension.

The mass analyser or ion trap may provide an ion flight path length of: between 5 and 15 m; between 6 and 14 m; between 7 and 13 m; or between 8 and 12 m.

The mass analyser or ion trap may provide an ion flight path length of: ≤20 m; ≤15 m; ≤14 m; ≤13 m; ≤12 m; or ≤11 m. Additionally, or alternatively, the mass analyser or ion trap may provide an ion flight path length of: ≥5 m; ≥6 m; ≥7 m; ≥8 m; ≥9 m; or ≥10 m. Any ranges from the above two lists may be combined where not mutually exclusive.

The mass analyser or ion trap may be configured to reflect or turn the ions N times in the oscillation dimension, wherein N is: ≥5; ≥6; ≥7; ≥8; ≥9; ≥10; ≥11; ≥12; ≥13; ≥14; ≥15; ≥16; ≥17; ≥18; ≥19; or ≥20. The mass analyser or ion trap may be configured to reflect or turn the ions N times in the oscillation dimension, wherein N is: ≤20; ≤19; ≤18; ≤17; ≤16; ≤15; ≤14; ≤13; ≤12; or ≤11. Any ranges from the above two lists may be combined where not mutually exclusive.

The spectrometer may have a resolution of: ≥30,000; ≥40,000; ≥50,000; ≥60,000; ≥70,000; or ≥80,000.

The spectrometer may be configured such that the pulsed ion accelerator receives ions having a kinetic energy of: ≥20 eV; ≥30 eV; ≥40 eV; ≥50 eV; ≥60 eV; between 20 and 60 eV; or between 30 and 50 eV. Such ion energies may reduce angular spread of the ions and cause the ions to bypass the rims of the orthogonal accelerator.

The spectrometer may comprise an ion detector.

The detector may be an image current detector configured such that ions passing near to it induce an electrical current in it. For example, the spectrometer may be configured to oscillate ions in the oscillation dimension proximate to the detector, inducing a current in the detector, and the spectrometer may be configured to determine the mass to charge ratios of these ions from the frequencies of their oscillations (e.g. using Fourier transform technology). Such techniques may be used in the electrostatic ion trap embodiments.

Alternatively, the ion detector may be an impact ion detector that detects ions impacting on a detector surface. The detector surface may be parallel to the drift dimension.

The ion detector may be arranged between the ion mirrors or sectors, e.g. midway between (in the oscillation dimension) opposing ion mirrors or sectors.

The present invention also provides a method of mass spectrometry comprising: providing a pulsed ion accelerator or mass spectrometer as described herein; and applying a pulsed voltage to at least one of said electrodes so as to pulse ions out of the ion accelerator, wherein the ions have a time front arranged in a first plane at the time the pulsed voltage is initiated, and wherein the ions pass through the wedge-shaped electric field region so as to cause the time front of the ions to be tilted at an angle to the first plane.

Herein there are proposed several ion optical elements, believed to be novel at least for MRTOF field:

I. A combination of a wedge pulsed field with post-acceleration in a “flat” (that is independent of the Z-coordinate) field. Such optical element, further referred as “amplifying wedge accelerator” appears a powerful, flexible and electrically adjustable tool for tilting time fronts of ion packets while introducing very minor ion ray steering;

II. A compensated deflector, incorporating quadrupolar field, e.g. produced by Matsuda plates. The compensated deflector overcomes the over-focusing of conventional deflectors in MPTOF, so as provides an opportunity for controlled ion packet focusing and defocusing; A set of compensated deflectors is used to bypass rims.

Further, the inventor has realized that applying a combination of compensated deflectors with amplifying wedge fields to MPTOF allows reaching: (a) spatial ion packet focusing Z|Z=0 onto detector; and (b) mutual compensation of multiple aberrations, including (i) first order time-front tilt T|Z, (ii) chromatic angular spread α/δ and, accounting analyzer properties, most of Y-related time-of-flight aberrations.

In application to orthogonal accelerators, there are achieved: (a) elevated energies of ion beams at the entrance of orthogonal accelerators for improved sensitivity and for reduced angular divergence Δα of ion packets; (b) dense folding of ion rays at small inclination angles for higher resolution of MPTOF.

The proposed schemes and some embodiments were tested and are presented here in ion optical simulations, which have verified the stated ion optical properties, including flexible tuning and compensation of misalignments; so as to confirm an ability of reaching a substantially improved combination of resolution and sensitivity within a compact MPTOF systems. As an example, FIG. 7 illustrates a compact 250×450 mm MRTOF system reaching resolution over 40,000.

Embodiments provide an ion injection mechanism into an isochronous electrostatic mass spectrometer, comprising:

(a) a pulsed acceleration stage with a wedge-type electric field;(b) a following static acceleration stage with a flat field;(c) at least one downstream ion deflector or a trans-axial deflector for ion ray steering;(d) wherein the initial mean ion energy prior to pulsed acceleration is much smaller compared to the ion energy within said at least one deflector; and(e) wherein the ion ray steering angle in said deflector and parameters of said accelerating stages are arranged and electrically adjusted to provide for mutual compensation of the ion packets time front tilt angle past said deflector.

Preferably, said at least one deflector may comprise means for generating an additional quadrupolar field for independent control over ion ray's steering angle and focusing or defocusing.

Preferably, said mass spectrometer may comprise at least one field-free space and at least one ion mirror and/or at least one electric sector.

Preferably, said mass spectrometer may comprise one of the group: (i) a time-of-flight mass spectrometer; (ii) an open ion trap; and (iii) an ion trap.

Embodiments provide a method of ion injection into an electrostatic field of an isochronous mass spectrometer, comprising the following steps:

(a) pulsed ion acceleration within a wedge-type electric field;(b) post-acceleration within a flat electrostatic field;(c) ion ray steering by at least one downstream ion deflecting field a trans-axial wedge deflecting field;(d) wherein the initial mean ion energy prior to pulsed acceleration is much smaller compared to the ion energy within said at least one deflector; and(e) wherein the ion ray steering angle in said deflector and parameters of said accelerating stages are arranged and electrically adjusted to provide for mutual compensation of the ion packets time-front tilt angle past said deflector.

Preferably, the method may further comprise a step of adding a quadrupolar field to said deflecting field for independent control over ion ray's steering angle and focusing or defocusing.

Preferably, said field of isochronous mass spectrometer may comprise at least one field-free space and at least one ion reflecting field of ion mirror and/or at least one deflecting field of electric sector.

Preferably, said field of mass spectrometer may be arranged for one type of mass spectral analysis of the group: (i) a time-of-flight mass analysis; (ii) an analysis of ion oscillation frequencies within an ion electrostatic trap or an open ion trap.

Embodiments provide an isochronous electrostatic mass spectrometer comprising:

(a) An ion source, generating ions;(b) An electrostatic analyzer substantially elongated in the first Z-axis and forming a two-dimensional electrostatic field in the orthogonal XY-plane for isochronous ion passage along a mean ion trajectory at an inclination angle α to the X-axis;(c) An ion accelerator with a pulsed accelerating stage, followed by a DC acceleration stage; said accelerator is arranged for emitting ion packets at an inclination angle α₀ to the X axis;(d) a time-of-flight detector or an image current detector;(e) At least one electrically adjustable electrostatic deflector for ion trajectory steering at angle ψ, associated with equal tilting of ion packets time front;(e) Wherein at least one electrode of said accelerator is tilted to the Z-axis to form an electrically adjustable wedge electrostatic field within said pulsed accelerating stage for adjusting of the time-front tilt angle γ of said ion packets relative to the Z-axis, associated with the steering of ion trajectories at smaller (relative to said angle γ) inclination angle φ;(f) Wherein said steering angles ψ and φ are arranged for either denser folding of major portion of ion trajectories at inclination angles α being smaller than said angle α₀, and/or for bypassing rims of said accelerator or deflector, and/or for reverting ion drift motion within said analyzer this way extending ion flight path and resolution; and(g) Wherein said time-front tilt angles γ and said ion steering angles ψ are electrically adjusted for mutual compensation of ion packets time front tilt angle at the detector plane, this way accounting unintentional misalignments of electrodes of the spectrometer.

Preferably, for the purpose of controlling spatial defocusing or focusing of said at least one deflector, an additional quadrupolar field may be formed within said deflector by at least one electrode structure of the group: (i) Matsuda plates; (ii) gate shaped deflecting electrode; (iii) side shields of the deflector with the aspect ratio under 2; (iv) toroidal sector deflection electrodes; and (v) additional electrode curvature within a trans-axial wedge deflector.

Preferably, said accelerator may be part of one pulsed ion source of the group: (i) a MALDI source; (ii) a SIMS source; (iii) a mapping or imaging ion source; and (iv) an electron impact ion source.

Preferably, said accelerator may be part of one pulsed converter of the group: (i) an orthogonal accelerator; (ii) a pass-through orthogonal accelerator with an electrostatic ion guide; and (iii) a radio-frequency ion trap with radial pulsed ion ejection.

Embodiments provide a method of time-of-flight mass spectral analysis comprising the following steps:

(a) generating ions in an ion source;(b) within an electrostatic analyzer substantially elongated in the first Z-axis, forming a two-dimensional electrostatic field in the orthogonal XY-plane for isochronous ion passage along a mean ion trajectory at an inclination angle α to the X-axis;(c) forming a pulsed accelerating field, followed by a DC acceleration field, arranged for emitting of ion packets at an inclination angle α₀ to the X axis;(d) detecting ions on a time-of-flight detector;(e) Ion trajectory steering at angle ψ, associated with equal tilting of ion packets time-front by least one electrically adjustable electrostatic deflector;(e) Forming an electrically adjustable wedge electrostatic field within said pulsed accelerating stage for adjusting of the time front tilt angle γ of said ion packets relative to the Z-axis, associated with the steering of ion trajectories at smaller (relative to said angle γ) inclination angle φ, arranged by tilting relative to the Z-axis of at least one electrode of said accelerator;(f) Wherein said steering angles ψ and φ are arranged for either denser folding of major portion of ion trajectories at inclination angles α being smaller than said angle α₀, and/or for bypassing rims of said accelerator or deflector, and/or for reverting ion drift motion within said analyzer this way extending ion flight path and resolution; and(g) Wherein said time-front tilt angles γ and said ion steering angles ψ are electrically adjusted for mutual compensation of ion packets time front tilt angle at the detector face, this way accounting misalignments of electrodes of spectrometer.

Preferably, for the purpose of controlling spatial defocusing or focusing of said at least one deflector, an additional quadrupolar field may be formed within said deflector by at least one electrode structure of the group: (i) Matsuda plates; (ii) gate shaped deflecting electrode; (iii) side shields of the deflector with the aspect ratio under 2; (iv) toroidal sector deflection electrodes; and (v) additional electrode curvature within a trans-axial wedge deflector.

Preferably, said ion acceleration step may be part of one pulsed ion step of the group: (i) a MALDI ionization; (ii) a SIMS ionization; (iii) an ionization with mapping or imaging of analyzed surfaces; and (iv) an electron impact ionization.

Preferably, said accelerator step may be part of one pulsed conversion step of the group: (i) an orthogonal acceleration; (ii) a pass-through orthogonal acceleration assisted by ion beam guidance by an electrostatic field of an ion guide; and (iii) a radio-frequency ion trapping with radial pulsed ion ejection.

BRIEF DESCRIPTION OF THE DRAWINGS

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

FIG. 1 shows prior art U.S. Pat. No. 6,717,132 planar multi-reflecting TOF with gridless orthogonal pulsed accelerator OA;

FIG. 2 illustrates problems of dense trajectory folding set by mechanical precision of the analyzer of FIG. 1;

FIG. 3 shows a novel deflector of an embodiment of the present invention, compensated by additional quadrupolar field for controlled spatial focusing;

FIG. 4 shows a novel wedge accelerator of an embodiment of the present invention, designed for flexible control over the tilt angle of ion packets' time front

FIG. 5 shows a balanced injection mechanism of an embodiment of the present invention employing the balanced deflector of FIG. 3 and wedge accelerator of FIG. 4 for controlling the inclination angle of ion packets while compensating the time-front tilt;

FIG. 6 shows numerical examples, illustrating ion packet spatial focusing within an MRTOF with the novel injection mechanism of FIG. 5, and presents a novel ion optical component of an embodiment of the present invention—a beam expander for bypassing detector rims, and demonstrates improved parameters of the exemplary compact MRTOF with resolution R>40,000;

FIG. 7 shows a numerical example with unintentional ion mirror misalignment—tilt of the ion mirror by 1 mrad, and illustrates how the novel injection mechanism of FIG. 5 helps compensating the misalignment with electrical adjustment of the instrument tuning;

FIG. 8 shows a sector MTTOF of an embodiment of the present invention with two improvements, one employing the compensated ion injection mechanism similar to FIG. 7, and the second employing a novel method the far-end ion packet steering with deflectors having quadrupolar focusing and defocusing fields of Matsuda plates; and

FIG. 9 shows alternative embodiments of pulsed ion sources and pulsed converters with novel amplifying wedge accelerating field.

DETAILED DESCRIPTION

Referring to FIG. 1, a prior art multi-reflecting TOF instrument 10 according to U.S. Pat. No. 6,717,132 is shown having an orthogonal accelerator (OA-MRTOF). The MRTOF instrument 10 comprises: an ion source 11 with a lens system 12 to form a substantially parallel ion beam 13; an orthogonal accelerator (OA) 14 with a storage gap to admit the beam 13; a pair of gridless ion mirrors 16, separated by field-free drift region, and a detector 17. Both OA 14 and mirrors 16 are formed with plate electrodes having slit openings, oriented in the Z-direction, thus forming a two dimensional electrostatic field, symmetric about the XZ symmetry plane (also denoted as s-plane). Accelerator 14, ion mirrors 16 and detector 17 are parallel to the Z-axis.

In operation, ion source 11 generates continuous ion beam. Commonly, ion sources 11 comprise gas-filled radio-frequency (RF) ion guides (not shown) for gaseous dampening of ion beams. Lens 12 forms a substantially parallel continuous ion beam 13, entering OA 14 along the Z-direction. Electrical pulse in OA 14 ejects ion packets 15. Packets 15 travel in the MRTOF analyser at a small inclination angle α to the x-axis, which is controlled by the ion source bias U_Z.

Referring to FIG. 2, simulation examples 20 and 21 are shown that illustrate multiple problems of prior art MRTOF instruments 10, if pushing for higher resolutions and denser ion trajectory folding. Exemplary MRTOF parameters were used, including: D_X=500 mm cap-cap distance; D_Z=250 mm wide portion of non-distorted XY-field; acceleration potential is U_X=8 kV, OA rim=10 mm and detector rim=5 mm.

In the Example 20, to fit 14 ion reflections (i.e. L=7m ion flight path) the source bias is set to U_Z=9V. Parallel ion rays with an initial ion packet length in the z-dimension of Z₀=10 mm and no angular spread Δα=0 start hitting rims of OA 14 and of detector 17. In Example 21, the top ion mirror is tilted by λ=1 mrad, representing realistic overall effective angle of mirror tilt, considering built up faults of stack assemblies, standard accuracy of machining and moderate electrode bend by internal stress at machining. Every “hard” ion reflection in the top ion mirror then changes the inclination angle α by 2 mrad. The inclination angle α grows from α₁=27 mrad to α2=41 mard, gradually expanding central trajectory. To hit the detector after N=14 reflections, the source bias has to be reduced to U_Z=6V. The angular divergence is amplified by mirror tilt and increase the ion packets width to ΔZ=18 mm, inducing ion losses on the rims. Obviously, slits in the drift space may be used to avoid trajectory overlaps and spectral confusion, however, at a cost of additional ionic losses.

In example 21, the inclination of ion mirror introduces yet another and much more serious problem. The time-front 15 of the ion packet becomes tilted by angle γ=14 mrad in front of the detector. The total ion packet spreading in the time-of-flight X-direction ΔX=ΔZ*γ=0.3 mm limits mass resolution to R<L/2ΔX=11,000 at L=7 m flight path, which is too low (for example compared to the desired R=80,000). To avoid the limitation, the electrode precision has to be brought to non-realistic level: λ<0.1 mrad, translated to better than 10 um accuracy and straightness of individual electrodes.

Summarizing problems of prior art MRTOF analysers, attempts of increasing flight path require much lower specific energies U_Z of the continuous ion beam and cause larger angular divergences Δα of the ion packets, which induce ion losses on component rims and may produce spectral overlaps. Importantly, small mechanical imperfections strongly affect MRTOF resolution and require unreasonably high precision.

Referring to FIG. 3, there is proposed a compensated deflector 30 to steer ion rays while overcoming the over-focusing effects of conventional deflectors by incorporating a quadrupolar field (e.g. E_Q=−2U_Qz/H²) in addition to the ion deflection field (e.g. E_Z=U/H). Conventional ion deflectors formed by opposing plate electrodes cause ions travelling at different positions between them to be deflected at different angles, causing angular dispersion of the ions and downstream over-focusing. The exemplary compensated deflector 30 according to embodiments of the present invention comprises a pair of deflection plates 32 spaced apart by distance H and having a potential difference U therebetween. The deflector 30 has side plates 33 at a different potential U_Q, known as Matsuda plates (e.g. in electrostatic sector fields). The additional quadrupolar field provides the first order compensation for angular dispersion that would be otherwise caused by the deflection plates 32 (i.e. as is problematic with conventional deflectors). The compensated deflector 30 is capable of steering ions by the same angle ψ (relative to its trajectory when entering the deflector) regardless of the Z-coordinate of the ion in the deflector, tilts the time front 31 by angle γ=−ψ, is capable of compensating the over-focusing (e.g. F→∞) while avoiding bending of the time front (such bending being typical for conventional deflectors), or alternatively is capable of controlling the focal distance F independent of the steering angle ψ.

ψ=D/2H*U/K; γ=−ψ=const(z)  (Eq. 1)

Alternatively, compensated deflectors may be used that are trans-axial (TA) deflectors, e.g. formed by wedge electrodes such as those described herein in relation to the pulsed orthogonal accelerator. By “compensated”, it is meant that the angular dispersion of the ions caused by the ion deflection may be compensated for, e.g. by the quadrupolar field. Embodiments of the invention propose using a first order correction, produced by an additional curvature of TA-wedge. Controlled focusing/defocusing may also be generated by combination of the TA-wedge and TA-lens, arranged separately or combined into a single TA-device. For a narrower range of deflection angles, the compensated deflector may be arranged with a single potential while selecting the size of Matsuda plates or with a segment of toroidal sector.

Compensated deflectors perform well with MRTOF or MPTOF analysers. The quadrupolar field in the Z-direction generates an opposite focusing or defocusing field in the transverse Y-direction. Below simulations prove that the focal properties of MPTOF analyzers are sufficient to compensate for the Y-focusing of deflectors 30 without any significant TOF aberrations.

Again referring to FIG. 3, an embodiment 35 with a pair of compensated deflectors 36 and 37 each comprise: a single deflecting plate 32, a shield 38 at drift potential and Matsuda plate 33. Deflectors 36 and 37 may be spaced by one ion reflection from an ion mirror 16. In other words, the ions may undergo only a single ion mirror reflection between passing through deflector 36 and deflector 37. Since Matsuda plates allow achieving both focusing and defocusing, the pair of deflectors 36 and 37 may be arranged for telescopic compression of ion packets 31 to 39 with the factor of compression being given by ΔZ₁/ΔZ₂=C1, achieved at mutual compensation of the time front steering angle γ=0, equivalent to T|Z=0 if adjusting steering angles as ψ₁=ψ₂*C1. Preferably pair of deflectors 36 and 37 provide for parallel-to-parallel ray transformation, which provides for mutual compensation of the time-front curvature, equivalent to T|ZZ=0. Then the compression factor of the second deflector 37 may be considered as C2=1/C1.

γ=0 and T|Z=0 at ψ₁=ψ₂*C1  (Eq. 2)

T|ZZ=0, if C1*C2=1  (Eq. 3)

Thus, using transformation of the Z-width of ion packets by compensated deflectors 37,37 allows adjusting the overall time front tilt angle after passing through a set of deflectors independent of the summary deflecting angle induced by this set.

Referring to FIG. 4, a novel orthogonal accelerator (OA) 40 according to an embodiment of the present invention is proposed, incorporating a wedge ion accelerating field in the area of stagnated ion packets, combined with a flat (that is independent of Z coordinate) ion accelerating field, thus forming an “amplifying wedge field”. The amplifying wedge field allows electronically controlling the tilt angle γ of ion packets' time front whilst introducing only a small steering angle ϕ of ion rays (relative to the x-axis).

An exemplary orthogonal accelerator 40 comprises: a region of pulsed wedge field 45, arranged between a tilted push electrode 44 and ground plate 47 aligned with the Z-axis; and a flat DC accelerating field 48 formed by electrodes parallel to the Z-axis. Field 48 may have accelerating and decelerating regions for producing low time spread and spatial ion focusing of ion packets (e.g. in the XY-plane), however, all equi-potentials of field 48 may stay parallel to the Z-axis.

In operation, a continuous ion beam 41 enters along the Z-axis at specific ion energy U_Z, e.g. defined by voltage bias of an upstream RF ion guide. Preferably ion beam angular divergence, spatial expansion and beam initial position are controlled by some radial confinement means that may be selected, for example, from the group of: (i) a radiofrequency rectilinear multipolar ion guide; (ii) an electrostatic quadrupolar ion guide with ion beam compression in the X-direction; (iii) an electrostatic periodic lens; and (iv) proposed in a co-pending application, an electrostatic ion guide with quadupolar field being spatially alternated along the Z-axis. An electrical pulse may be applied periodically to the push plate 44, ejecting a portion of the beam 41 through an aperture in electrode 47, thus forming an ion packet with starting time-front 42, which crosses a starting equipotential 46 that is tilted at the angle λ₀ to the x-axis. Ions start with zero mean energy in the X-direction K=0, at the exit of wedge field 45 ions gain specific energy K₁ and at the exit of DC field 48 gains the energy K₀. Assuming small angles λ₀ of equipotential 46 (in further examples 0.5 deg), beam thickness of at least ΔX>1 mm and moderate ion packet length (examples use Z₀=10 mm), the λ₀ tilt of starting equipotential 46 produces negligible corrections onto energy spread of ions in the x-direction ΔK of ion packet 49.

By applying trivial mathematics a non-expected and previously unknown result was arrived at: in accelerator 40 with amplifying wedge accelerating field, the time front tilt angle relative to the z-axis (γ) and the ion steering angle ϕ=introduced by the wedge field are controlled by the energy factor K₀/K₁ as:

γ=2λ*(K₀/K₁)^0.5=2λ*u₀/u₁  (Eq. 4)

ϕ=2λ/3*(K₁/K₀)^0.5=2λ/3*u₁/u₀  (Eq. 5)

i.e. γ/ϕ=3K₀/K₁>>1  (Eq. 6)

where K₁ and K₀ are mean ion kinetic energies at the exit of the wedge field 45 (index 1) and at the exit of flat field 48 (index 0) respectively, and u₁ and u₀ are the corresponding mean ion velocities.

Thus, novel accelerators with amplifying wedge field allow (i) operating with (e.g. continuous) ion beams introduced along the Z-axis, which allows convenient instrumental arrangements; (ii) tilting ion packets time front to a substantial angle γ, which may then be used for compensation of the time-front tilt in one or more ion deflector; (iii) controlling tilt angle electronically, either by adjusting the pulse potential or by minor steering of the (e.g. continuous) ion beam between various starting equipotential lines.

Again referring to FIG. 4, similar embodiment 40TR is proposed for an ion trap converter, having the same (as embodiment 40 OA) reference numbers for accelerator components. The trap 40TR may be arranged for ion through passage or for ion trapping in the Z-direction, where 41 is either an ion beam or an ion cloud correspondingly. In both cases one of the same (as in 40OA) means for radial ion confinement may be used, for example: (i) a radiofrequency rectilinear multipolar ion guide; (ii) an electrostatic quadrupolar ion guide with ion beam compression in the X-direction; (iii) an electrostatic periodic lens; or (iv) proposed in a co-pending application, an electrostatic ion guide with quadupolar field being spatially alternated along the Z-axis.

Ion injection into an MRTOF analysers may be improved by using higher energies of continuous ion beam for improving the ion beam admission into an orthogonal accelerator (OA) and for reducing angular divergence of ion packets in the MRTOF analyser. For higher MRTOF resolution, ion trajectories may be compact folded by using back steering of ion packets, achieved with a deflector. To compensate for the time front tilt produced by the deflector, it is proposed to use an amplifying wedge accelerating field such as that described above in the OA.

Referring to FIG. 5, embodiments 50 of the ion injection mechanism into the MRTOF analyser of embodiments of the present invention comprise: a planar ion mirror 53 with 2D XY-field, extended in the Z-direction; an orthogonal accelerator 40 with “flat” DC acceleration field 48 aligned with Z-axis and a wedge accelerating field 45 produced by tilted push plate 44; and a compensated deflector 30, located along the ion path and after first ion mirror reflection. Deflector 30 may correspond to the one of FIG. 3 and the accelerator 40 may correspond to one of those in FIG. 4.

The operation of embodiment 50 is illustrated by simulation example 51, showing time fronts 54 and 55 crossing ion rays. Continuous ion beam 41 at specific energy (e.g. U_Z=57V) propagates along the Z-axis to cross starting (K=0) equipotential 46, which is tilted at the angle λ₀ (e.g. λ₀=0.5 deg) to the z-axis, with push plate 44 being tilted by 1 deg to the z-axis. Pulsed wedge field 45 accelerates ions to mean energy K₁ (e.g. K₁=800V), and flat field 48 to K₀ (e.g. K₀=8 kV), thus producing an amplifying factor K₀/K₁≅10. The amplifying wedge tilts the ion packets time front 54 at a large angle [e.g. γ=2λ₀*(K₀/K₁)^0.5≅6λ₀], while having a small deflection effect on the trajectory of the ion ray relative to the x-axis (as compared to if a conventional non-wedged and untilted OA was used). For example, the OA may result in an angle α₁=α₀−ϕ=4.7 deg (where ϕ≅0.2 deg is the deflection angle caused by the wedged field). In other words, the ion rays are inclined almost at natural inclination angle α₀=(U_Z/U_X)^0.5=4.9 deg.

After the first ion mirror reflection, deflector 30 steers ion rays by angle ψ=−γ=−3.2 deg (in the x-z plane), thus reducing the inclination angle to the x-direction to α₂=α₁−ψ=1.5 deg, while aligning the ion packets time front 55 parallel with the Z-axis, i.e. γ=0. Much higher specific energies of the ion beam (e.g. U_Z=57V as compared to 9V in the prior art) improves the ion admission into the OA and reduces the angular divergence Δα of ion packets, allowing denser folding of ion trajectories at smaller inclination angles, e.g. here at α₂=α₁−ψ=1.5 deg (as compared to the natural inclination angle α₀=4.9 deg).

Table 1 below summarizes the equations for angles within the individual deflector 30 and wedge accelerator 40. Table 2 below presents conditions for compensation of the first order time-front tilt (T|Z=0) and of the chromatic spread of Z-velocity (α|K=0). It is of significant importance that both compensations are achieved simultaneously. This is a new finding by the inventor. The pair of wedge accelerator 40 and deflector 30 compensate multiple aberrations, including the first order time front tilt, the chromatic angular spread and, accounting focusing properties of gridless ion mirrors in example 51, the angular and spatial spreads of ion packets in the Y-direction.

TABLE 1
			Chromatic
			dependence of
	Time-front	Rays Steering	Z-velocity
	Tilt Angle	Angle	d(Δw)/dδ
Wedge Accelerator	${\gamma }_0^{\left(OA\right)}=2{\lambda }_0\sqrt{\frac{K_0}{K_1}}$	${\phi }^{\left(\mathrm{OA}\right)}\approx +\frac{2{\lambda }_0}{3}\sqrt{\frac{K_1}{K_0}}$	${\lambda }_0{u}_0\sqrt{\frac{K_0}{K_1}}$
Deflector	−ψ0	ψ0	$-\frac{1}{2}{u}_0{\psi }_0$

TABLE 2
	Condition for the 1st order Time-	Condition for Compensating
	front Tilt Compensation	Chromatic Spread of Z-velocity
Wedge Accelerator + Deflector	$2\lambda \sqrt{\frac{K_0}{K_1}}={\psi }_0$	$2\lambda \sqrt{\frac{K_0}{K_1}}={\psi }_0$

Referring back to FIG. 5, an alternative embodiment 52 differs from embodiment 50 by tilting DC acceleration field 48 relative to the z-axis by angle λ₀ for aligning ion beam 41 parallel with starting equi-potential 46. Although the angles are shifted, however, the above described compensations survive.

Referring to FIG. 6, the compensated mechanism 50 of ion injection into the MRTOF analyser has been verified in ion optical simulations 60, 62, 64 and 66. An exemplary MRTOF analyser comprises an ion mirrors 53 with cap-cap distance in the x-dimension of D_X=450 mm and useful width in the z-dimension of D_Z=250 mm, operating at acceleration potential in the x-dimension of U_X=8 kV. Examples of FIG. 6 employ compensated deflector 30 with the Matsuda plates of FIG. 3, amplifying wedge accelerator 40 of FIG. 4, dual deflector 30D with Matsuda plates, and TOF detector 17, assumed having DET=1.5 ns Gaussian signal spread. Similar to example 51, continuous ion beam of μ=1000 amu with ΔX=1 mm width and 2 deg full angular divergence enters wedge OA at U_Z=57V specific (per charge) energy and ΔU_Z=0.5V energy spread.

Example 60 illustrates spatial focusing of ion rays 61 for ion packets having an initial width in the z-dimension of Z₀=10 mm, while not accounting angular spread of ion packets Δα=0 at ΔU_Z=0 and not accounting relative energy spread of ion packets δ=ΔK/K=0 at ΔX=0. The chosen position of deflector 30 improves the ion packets bypassing of the deflector 30. The Matsuda plate voltage of the deflector 30 is electrically adjusted for geometrical focusing of ion packets onto the detector, which allows a denser folding of ion rays in MRTOF at α₂=1.5 deg.

Example 62 illustrates angular divergence of ion rays 63 at ΔU_Z=0.5V, while not accounting ion packets width Z₀=0 and energy spread δ=0. Dual compensated deflector 30D (another novel component for MRTOF) helps spreading ion rays in-front of the detector 17 for bypassing the detector rims (here 5 mm).

Example 64 illustrates the (predicted by Table 4) simultaneous compensation of chromatic angular spread α|δ=0 and of the first order time-front tilt γ=0 at δ=0.05, ΔU_Z=0, and Z₀=0. Dark areas along the ion trajectories show lengths of ion packets due to the energy spread at equally spaced time intervals, and in particular time focusing after each reflection and at the detector.

Example 66 illustrates overall mass resolution R_M=47,000 achieved in a compact 450×250 mm analyzer while accounting all realistic spreads of ion beam and ion packets, so as DET=1.5 ns time spread. The embodiment satisfies a goal of R>40,000 for resolving major isobars for μ=m/z<500 in GC-MS instruments.

Apparently, the injection mechanism 50 has a built-in and not yet fully appreciated virtue—an ability to compensate for mechanical imperfections of the MRTOF analyser by electrical tuning of the instrument, including adjustment of ion beam energies U_Z, the pulse voltage on push plate 44, deflector 30 steering, or steering of continuous ion beam 41 to fit different equi-potentials 46.

Referring to FIG. 7, there is presented a simulation example 70, employing the MRTOF analyzer of FIG. 6 with D_X=450 mm, D_Z=250 mm, and U_X=8 kV. The example 70 is different from 60 by introducing a Φ=1 mrad tilt of the entire top mirror 71, representing a typical non intentional mechanical fault at manufacturing. If using the tuned settings of FIG. 6, resolution drops to 25,000 as shown in the graph 74. The resolution may be partially recovered to R=43,000 as shown in icon 75 by increasing the source bias and specific energy of continuous ion beam from U_Z=57V to U_Z=77V, and by retuning deflectors 30 and 30D. Example 70 shows ion rays after the compensation when accounting for all realistic ion beam and ion packet spreads, similar to FIG. 6. Thus, the proposed injection scheme 50 into a compact MRTOF allows compensating for moderate mechanical misalignments and recovering MRTOF resolution by electrical adjustments.

Referring to FIG. 8, an embodiment of a sector MTTOF analyser 80 of the present invention is shown, together with simulation examples 86, 87 and 88. The analyser comprises: sectors 82 and 83, separated by a drift space; an orthogonal accelerator 40 of FIG. 4, a compensated deflector 30 of FIG. 3; and a pair of compensated deflectors 84 and 85, similar to 30, however having different voltage settings of their Matsuda plates.

Electrodes of sectors 82 and 83 are extended in the Z-direction to form two-dimensional fields in the XY-plane, i.e. they do not have laminating fields of the prior art. Sectors 82 and 83 have different radii and are arranged for isochronous cycled trajectory 81 (well seen in the view 86) with at least second order time per energy focusing, as described in WO (RMS).

As shown in view 87, continuous ion beam 41 propagates along the Z-axis at elevated specific energy U_Z (expected from 20 to 50V). A compensated ion injection mechanism into MTTOF 80 is arranged with a wedge accelerator 40 and compensated deflector 30, similar to injection mechanism 50, described in FIG. 5. Accelerator 40 with amplifying wedge accelerating field tilts the time front 89 of ion packets to compensate for the time front tilt of the downstream deflector 30, thus arranging dense trajectory folding at small inclination angles α₂ while using relatively higher injection energies U_Z. Ion packets bypass the OA 40 at larger angle α₁ and then advance in the drift Z-direction within MTTOF along the spiral trajectory 81 at reduced inclination angle α₂. Thus, a combination of wedge accelerator and of compensated deflector is well suitable for sector MTTOF analysers.

Embodiment 80 presents yet another novel ion optical solution—a compensated reversing of ion trajectories in the drift Z-direction. The idea of time front compensation after reversing is similar to that shown in arrangement 35 of FIG. 3. The reversing mechanism is arranged with a pair of focusing and defocusing deflectors 84 and 85, best seen and explained in simulation example 88, for clear view expanded in the Z-direction. Ion packets reach far Z-end of the sector analyzer at an inclination angle α₂. Deflector 84 with Matsuda plates is set for increasing the inclination angle to α₃ while focusing the packet Z-width within deflector 85. Deflector 85 is set to reverse ion trajectory with deflection for −2α₃ angle and defocuses the packet from Z₃ to Z₂ by using Z-defocusing quadrupolar field of Matsuda plates in deflector 85. The focusing factor Z₃/Z₂ and deflection angles are arranged as 2Z₃*α₃=Z₂(α₃−α₂) to mutually compensate for the time-front tilts, as illustrated with simulated dynamics of the time front 89. The proposed method of compensated reversing of ion trajectories is suitable for both MRTOF and MTTOF analyzers.

Referring to FIG. 9, exemplary embodiments 90, 92, 94, 96 and 98 of the present invention illustrate a variety of alternative pulsed ion sources and pulsed converters with amplifying wedge field 45, arranged for electronically adjustable tilt of time-fronts 54. All examples comprise a wedge field region 45, arranged within the region of small ion energy, and a flat post-acceleration field 48 for amplification of the tilt angle γ of time-front 54, preferably accompanied with notably smaller steering angle ϕ of ion trajectories. The time front tilt γ may be arranged for compensation of the time front steering associated with the downstream trajectory steering for angle ψ, about matching the angle γ for mutual compensation. Similar to previous drawings, ion starting equi-potentials are denoted as 46 and compensated deflectors are denoted by 30.

Deflectors 30 may be arranged anywhere downstream of the accelerator, which is illustrated by dashed ion rays between accelerator and deflector 30. However, to reduce the effect of ion packet angular divergence on compensation of time-front tilt, it is preferable to keep deflector 30 either immediately after the accelerator or after the first ion mirror reflection, or after the first electrostatic sector turn, or within the first full ion turn.

Example 90 presents an alternative spatial arrangement of the wedge accelerating field 45. An intermediate electrode 91 is tilted to produce the wedge at earlier stages of ion acceleration, though not immediately at ion starting point. Adjusting the potential of electrode 91 allows controlling the time front tilt angle γ electronically.

Example 92 presents an arrangement with an intermediate printed circuit board 93, having multiple electrode segments (in the x-direction) that are interconnected via a resistive chain for generating a wedge field structure similar to that in embodiment 90. The PCB embodiment 92 may provide a yet wider range of γ electronic tuning than 90.

Example 94 illustrates an application of the wedge accelerator to pulsed EI sources. Example 94 comprises an electron gun 95 and magnets B for controlling electron beam direction. Optionally, magnets may be tilted to align the electron beam with the tilted equipotential 46. Diverging electrodes within the EI source reduce the risk of electrode contamination by electron bombardment. Ions are produced by electron impact and are stored within the space charge field of the electron beam. Periodically electrical pulses are applied to tilted electrode 44. Example 94 provides compensated steering of ion rays past EI source, e.g. in order to bypass the accelerator and to adjust the inclination angle α of ion trajectories within an MRTOF or MTTOF analyser. The Matsuda plate potential in deflector 30 may be adjusted to control the ion packet spatial focusing.

Example 96 presents the application of the wedge accelerator to radio-frequency (RF) trap converters with radial ion ejection, known for their high (up to unity) duty cycle of pulsed conversion. The converter comprises side electrodes 97 at RF signal. The structure of electrodes 97 is better seen in the XY-plane. Ions are injected into the trap axially (in the x-direction) and are retained aligned with electrode 97 by the confining quadrupolar RF field of electrodes 97. In one (through) mode, the beam may propagate along equipotential 46 at small energy. In another (trapping) mode ions may be slowly dampened by gas at moderate mid-vacuum pressure (e.g. around 1 mTorr within several ms time). Ion packets are periodically ejected by energizing push plate 44. Tilting of push plate 44 controls the time-front tilt γ, which may be produced for compensating the downstream steering of time fronts by deflector 30. Example 96 provides compensated steering of ion rays past radial traps, e.g. in order to bypass the trap and to adjust the inclination angle α of ion trajectories within MRTOF or MTTOF analysers. The Matsuda plate potential in deflector 30 may be adjusted to control the ion packet spatial focusing. Note that to compensate T|ZZ aberrations at focusing in deflector 30 of substantially elongated ion packets, an additional compensating field curvature may be generated within accelerating field 45, either by curving electrode 97, or by curving of other trap electrodes, or by auxiliary fringing field, penetrating through or between trap electrodes.

Example 98 presents the application of the wedge accelerator to surface ionization methods, such as MALDI, SIMS, FAB, or particle bombardment, defined by the nature of primary beam 99—either photons, or pulsed packets of primary ions, or neutral particles or glow discharge or heavy particles or charged droplets. Electrode 44 may be energized static or pulsed, depending on the overall arrangement of prior art ionization methods. It is assumed that the exposed surface is relatively wide, either for imaging purposes or for improved sensitivity, so that ion packet width does affect the time-of-flight resolution, if ion packets are steered without compensation. Arranging wedge accelerator field 45, for example by tilting the target 44, is used here for compensating the time front tilt steering or for the spatial focusing of ion packets, or as a part of the surface imaging ion optics. Benefits of example 98 may be immediately seen by experts such as: (a) steering of ion packets allows the ion source bypassing and denser folding of ion trajectory in MPTOF analysers; (b) focusing by deflector 30 improves sensitivity; (c) unintentional tilt of the target 44 or some uneven topology of the sample on the target may be compensated electronically; (d) ion steering off the source axis allows an orthogonal arrangement of the impinging primary beam 99A; (e) compensated edge and curvature of accelerating field may be used for improving stigmatic properties of the overall imaging ion optics. Some further benefits are likely to be found, since the scheme allows fine and electronically adjustable control over the spatial focusing and the time-of-flight aberrations of the surface ionizing sources.

Annotations

Coordinates and Times:

x,y,z—Cartesian coordinates;X Y, Z—directions, denoted as: X for time-of-flight, Z for drift, Y for transverse;Z₀—initial width of ion packets in the drift direction;ΔZ—full width of ion packet on the detector;D_X and D_Z—used height (e.g. cap-cap) and usable width of ion mirrorsL—overall flight pathN—number of ion reflections in mirror MRTOF or ion turns in sector MTTOFu—x-component of ion velocity;w—z-component of ion velocity;T—ion flight time through TOF MS from accelerator to the detector;ΔT—time spread of ion packet at the detector;

Potentials and Fields:

U—potentials or specific energy per charge;U_Z and ΔU_Z—specific energy of continuous ion beam and its spread;U_X—acceleration potential for ion packets in TOF direction;K and ΔK—ion energy in ion packets and its spread;δ=ΔK/K—relative energy spread of ion packets;E—x-component of accelerating field in the OA or in ion mirror around “turning” point;μ—m/z—ions specific mass or mass-to-charge ratio;

Angles:

α—inclination angle of ion trajectory relative to X-axis;Δα—angular divergence of ion packets;γ—tilt angle of time front in ion packets relative to Z-axisλ—tilt angle of “starting” equipotential to axis Z, where ions either start accelerating or are reflected within wedge fields of ion mirrorθ—tilt angle of the entire ion mirror (usually, unintentional);φ—steering angle of ion trajectories or rays in various devices;ψ— steering angle in deflectorsε—spread in steering angle in conventional deflectors;

Aberration Coefficients

• T|Z, T|ZZ, T|δ, T|δδ, etc;

indexes are defined within the text

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

Claims

1. A mass spectrometer having a pulsed ion accelerator, said pulsed ion accelerator comprising: a plurality of electrodes arranged and configured to generate an ion pulsing region, wherein the pulsed ion accelerator is configured such that ions entering the ion accelerator are initially received in the ion pulsing region; anda plurality of electrodes arranged and configured to generate a wedge-shaped electric field region downstream of said ion pulsing region;wherein the pulsed ion accelerator is configured to apply a pulsed voltage to at least one of said electrodes of the ion pulsing region for pulsing ions out of the ion accelerator, wherein the ions have a time front arranged in a first plane at the time the pulsed voltage is initiated, and wherein the ion accelerator is configured such that the pulsed ions pass through the wedge-shaped electric field region so as to cause the time front of the ions to be tilted at an angle to the first plane;wherein the ion accelerator further comprises a plurality of electrodes arranged and configured to generate an ion acceleration region downstream of the wedge-shaped electric field region for amplifying the time front tilt introduced by the wedge-shaped electric field; andwherein the at least one of said electrodes of the ion pulsing region for pulsing ions out of the ion accelerator is substantially parallel to said electrodes of the ion acceleration region.

2. The mass spectrometer of claim 1, wherein said plurality of electrodes for generating said ion acceleration region are a plurality of parallel electrodes.

3. The mass spectrometer of claim 1, wherein said electrodes for generating said wedge-shaped electric field region are arranged and configured for generating said wedge-shaped electric field region therebetween such that equipotential field lines in the wedge-shaped electric field region are angled to each other so as to form the wedge-shape.

4. The mass spectrometer of claim 1, wherein said electrodes for generating said wedge-shaped electric field region comprise one or more first electrode arranged in a first plane and one or more second electrode arranged in a second plane that is angled to the first plane so as to define the wedge-shaped electric field region between the one or more first electrode and one or more second electrode.

5. The mass spectrometer of claim 1, wherein said electrodes for generating said wedge-shaped electric field region comprise one or more first electrode arranged in a first plane and a plurality of second electrodes arranged in a second plane, wherein the ion accelerator is configured to apply different voltages to different ones of the second electrodes so as to define the wedge-shaped electric field region between the one or more first electrode and the second electrodes, wherein the second plane is parallel to the first plane.

6. The mass spectrometer of claim 5, wherein the pulsed ion accelerator comprises a printed circuit board which provides the second electrodes.

7. The mass spectrometer of claim 1, wherein the electrodes for generating said wedge-shaped electric field region are arranged so that equipotential field lines of the wedge-shaped electric field extend substantially in a first direction and the plurality of electrodes for generating an ion pulsing region are configured to pulse the ions through the wedge-shaped electric field substantially transverse to the equipotential field lines.

8. The mass spectrometer of claim 1, wherein the ion accelerator is arranged and configured to receive ions travelling in a first direction along a first axis that is substantially parallel to equipotential field lines of the wedge-shaped electric field.

9. The pulsed ion accelerator of claim 1, wherein said electrodes of the ion acceleration region are configured to apply a static electric field in the ion acceleration region for accelerating the ions.

10. The pulsed ion accelerator of claim 1, wherein said electrodes of the ion acceleration region are configured to apply an electric field in the ion acceleration region having parallel equipotential field lines for accelerating the ions.

11. The mass spectrometer of claim 1, comprising an ion optical component located downstream of the pulsed ion accelerator which deflects the average ion trajectory of the ions, thereby tilting the angle of the time front of the ions by the ion optical component; and wherein the wedge-shaped electric field region of the pulsed ion accelerator is configured to tilt the time front of the ions passing therethrough so as to at least partially counteract the tilting of the time front by the ion optical device.

12. The mass spectrometer claim 1, wherein said pulsed ion accelerator is one of: (i) a MALDI source; (ii) a SIMS source; (iii) a mapping or imaging ion source; (iv) an electron impact ion source; (v) a pulsed converter for converting a continuous or pseudo-continuous ion beam into ion pulses; (vi) an orthogonal accelerator; (vii) a pass-through orthogonal accelerator having an electrostatic ion guide; or (viii) a radio-frequency ion trap with pulsed ion ejection.

13. The mass spectrometer of claim 1, comprising: a multi-pass time-of-flight mass analyser or electrostatic ion trap having the pulsed ion accelerator, and electrodes arranged and configured so as to provide an ion drift region that is elongated in a drift direction (z-dimension) and to reflect or turn ions multiple times in an oscillating dimension (x-dimension) that is orthogonal to the drift direction.

14. The mass spectrometer of claim 13, wherein: (i) the multi-pass time-of-flight mass analyser is a multi-reflecting time of flight mass analyser having two ion mirrors that are elongated in the drift direction (z-dimension) and configured to reflect ions multiple times in the oscillation dimension (x-dimension), wherein the pulsed ion accelerator is arranged to receive ions and accelerate them into one of the ion mirrors; or(ii) the multi-pass time-of-flight mass analyser is a multi-turn time of flight mass analyser having at least two electric sectors configured to turn ions multiple times in the oscillation dimension (x-dimension), wherein the pulsed ion accelerator is arranged to receive ions and accelerate them into one of the sectors.

15. The mass spectrometer of claim 13, comprising an ion deflector located downstream of said pulsed ion accelerator, and that is configured to back-steer the average ion trajectory of the ions, in the drift direction, thereby tilting the angle of the time front of the ions received by the ion deflector.

16. The spectrometer of claim 15, wherein the wedge-shaped electric field region of the pulsed ion accelerator is configured to tilt the time front of the ions passing therethrough so as to at least partially counteract the tilting of the time front by the ion deflector.

17. The spectrometer of claim 15, wherein the ion deflector is configured to generate a quadrupolar field for controlling the spatial focusing of the ions in the drift direction.

18. The mass spectrometer of claim 1, wherein said electrodes of the ion pulsing region for pulsing ions out of the ion accelerator are substantially parallel to said electrodes of the ion acceleration region, and wherein said electrodes for generating said wedge-shaped electric field region comprises an intermediate electrode tilted at an angle to the electrodes of the ion pulsing and ion acceleration regions so as to define the wedge-shaped electric field.

19. The mass spectrometer of claim 1, wherein said electrodes of the ion pulsing region are configured for pulsing ions in a pulse direction, wherein said pulsed ion accelerator comprises a printed circuit board which provides said electrodes for generating said wedge-shaped electric field region, said electrodes for generating said wedge-shaped electric field region comprise multiple electrode segments (in the pulsing direction) that are interconnected via a resistive chain for generating said wedge-shaped electric field region.

20. A method of mass spectrometry comprising: providing the mass spectrometer as claimed in claim 1;applying the pulsed voltage to the plurality of electrodes for generating said ion pulsing region so as to pulse ions out of the ion accelerator, wherein the ions have a time front arranged in the first plane at the time the pulsed voltage is initiated, and wherein the ions pass through the wedge-shaped electric field region so as to cause the time front of the ions to be tilted at the angle to the first plane.