Patent Application
20230170205
The invention lies in the field of charged particle detectors. In particular, it relates to a high-performance apparatus for detecting charged particles, which finds application among others in Mass Spectrometry, including Secondary Ion Mass Spectrometry, SIMS.
Mass spectrometry is an analytical technique that is commonly used to determine the elements that compose a molecule or sample. A mass spectrometer typically comprises a source of ions, a mass separator and a detector. The source of ions may for example be a device that is capable of converting the gaseous, liquid or solid phase of sample molecules into ions, that is, electrically non-neutral charged atoms or molecules. Several ionization techniques are well known in the art, and the particular structure of an ion source device will not be described in any detail in the present specification. Alternatively, the ions to be analyzed by the mass spectrometer may result from the interaction between the sample in its gaseous, liquid or solid phase and an irradiation source, such as a laser, ion or electron beam. The ion-emitting sample is in that case considered to be the source of ions.
The ion beam that originates at the ion source is analyzed using a mass analyzer, which is capable of separating, or sorting, the ions according to their mass-to-charge ratio. The ratio is typically expressed as m/z, wherein m is the mass of the analyte in unified atomic mass units, and z is the number of elementary charges carried by the ion. The Lorentz force law and Newton's second law of motion in the non-relativistic case characterize the motion of charged particles in space. Mass spectrometers therefore employ electrical fields and/or magnetic fields in various known combinations in order to separate the ions emanating from the ion source. An ion having a specific mass-to-charge ratio follows a specific trajectory in the mass-analyzer. As ions of different mass-to-charge ratios follow different trajectories, the composition of the analyte may be determined based on the observed trajectories. By analogy with an optical spectrometer, which allows generation of a spectrum of the different wavelengths comprised in a wave beam, the mass spectrometer allows for generating a spectrum of the different mass-to-charge ratios comprised in a molecule or sample.
Sector instruments are a specific type of mass analyzing instrument. A sector instrument uses a magnetic field or a combination of an electric and magnetic field to affect the path and/or velocity of the charged particles. In general, the trajectories of ions are bent by their passage through the sector instrument, whereby light and slow ions are deflected more than heavier fast ions. Magnetic sector instruments generally belong to two classes. In scanning sector instruments, the magnetic field is changed, so that only a single type of ion is detectable in a specifically tuned magnetic field. By scanning a range of field strengths, a range of mass-to-charge ratios can be detected sequentially. In non-scanning magnetic sector instruments, a static magnetic field is employed. A range of ions may be detected in parallel and simultaneously. The known non-scanning magnetic sector instruments are typically classified as Mattauch-Herzog type mass spectrometers.
A Mattauch-Herzog type mass analyzer consists of an electrostatic sector, ESA, followed on the secondary ion trajectories by a magnetic sector. The arrangement of the electrostatic sector and the magnetic sector typically allows to disperse a wide range of mass-to-charge ratios m/z along the exit plane of the magnetic sector. All the ion masses are focused on a focal plane located at the exit plane (in the original Mattauch-Herzog configuration), or at a distance from the exit plane of the magnetic sector. Most of the known Mattauch-Herzog type mass spectrometers are able to operate in the double focusing condition (achromatic mass filtering) for the highest mass resolving power. A typical mass resolving power from hundreds to thousands are achieved.
One interesting features of this mass spectrometer architecture is its capability to capture simultaneously a wide range of the mass spectrum, provided that it is equipped with an appropriate detection system, ideally comprising a focal plane detector. A focal plane detector is able to simultaneously acquire the full mass spectrum in a short acquisition time, typically in a fraction of a second. This simultaneous acquisition capability offers several benefits. Firstly, a measurement duty cycle of 100% can be achieved. This benefit can result in better detection limits as well as smaller sample sizes needed for the measurement since all the mass-to-charge ratio (m/z) peaks are collected at the same time. Secondly, the ability to simultaneously record the entire mass spectrum allows for using both continuous and pulsed ionization techniques. In particular, the pulsed ionization techniques such as laser ablation/ionization commonly introduce rapid changes in the spectrum signal and therefore sequential detection techniques would cause errors in the measurements.
An ideal focal plane detector for mass spectrometry should be sensitive enough to detect a single ion while the count rate of its single 1-dimensional (1D) pixel (local count rate) should be more than 107 counts per seconds, cps, in order to handle the highest ion beam currents. In practice, a 1D local count rate of more than 106 cps/mm is typically required. Furthermore, the local dynamic range (defined by the signal range in which the detector responds linearly to the detected signal) is also required to be 105-106 in order to accurately measure a wide range of chemical concentrations.
Known detection systems typically comprise at least one microchannel plate, MCP, unit. A typical microchannel plate, MCP, is composed of 104 to 107 miniature electron multipliers whose typical diameters are in the range from 10 to 100 μm. Each channel acts as an individual electron multiplier, which can detect a single ion, electron, atom, molecule or photon. The MCP is typically fabricated from a high resistive material such as lead glass. The front side and rear side of the MCP are metallized electrodes to which a typical voltage difference of about 1000V is applied through appropriate biasing means, such as a source of electricity. When a single energetic particle hits a channel surface, it creates one or more secondary electrons, which are accelerated into an MCP channel by the applied voltage. Each of these secondary electrons can release two or more secondary electrons when hitting the channel wall again. This process is cascaded along the channel Therefore, a single energetic particle hitting a channel creates a cascade of electron emission along the channel, resulting in an electron cloud of at least 104 electrons at the output of the channel. An anode placed behind the MCP can electronically detect the electron cloud to register each single event hitting the MCP. An MCP assembly may comprise a single microchannel plate, or a stacked assembly thereof.
Known MCP-based focal plane detectors, are however plagued by several limitations. A limited local count rate results in the detection signal being saturated for high concentration species. Typical MCPs limit the local count rate to 104-105 cps/mm2. In known MCP-based focal plane detectors, this local count rate of the MCP limits the 1D local count rate to less than 104-105 cps/mm. A limited local dynamic range results in poor detectable concentration range of the species. Mass spectrometry typically requires a wide range of dynamic range up to greater than 106. Although the overall dynamic range of known MCP devices is typically greater than 107, the local dynamic range that it allows is hundreds to thousands of times smaller (103-104).
The above two limitations of the MCP-based technologies are mainly due to the fact that each MCP channel is limited by a maximum count rate that it can handle, and therefore the maximum local count rate and local dynamic range of one detector pixel are dependent on the number of MCP channels involved in the pixel. Each MCP channel is typically characterized by a dead time of several milliseconds between two detection events and therefore the maximum count rate that a MCP channel can handle is limited to less than 102 cps. Depending on the size of MCP channel, the density of the MCP is typically from 103 to less than 104 channels/mm2. Considering the statistics for avoiding multiple ions hitting the same channel, the maximum count rate of a single MCP is limited to maximum 105 cps/mm2 or less. This limited count rate is typically worse in the MCP stack configurations, where two or three MCPs are joined together in order to improve the overall gain. In this case, a single particle hitting a channel of the first MCP can result in a dead time for several channels of the following MCP plates involved in the detection of this single particle. Therefore, the achievable maximum count rate in such known architecture is much less than 104-105 cps/mm2, and the local dynamic range is much less than 104 (considering a minimum signal to noise ratio that is larger than 3).
Patent document U.S. Pat. No. 6,521,887 B1 discloses a Time-of-Flight, TOF, spectrometer. It aims at avoiding a pulsed or gated ion beam in order to increase the TOF instrument's duty cycle. Deflection means in the drift region of the instrument are used to deviate the single ion beam to different positions on a detection device, that may comprise an MCP assembly.
It is an objective of the invention to present a device, which overcomes at least some of the disadvantages of the prior art. In particular, the invention aims at providing a charged particle detection apparatus, which yields improved performance over known MCP-based charged particle detectors.
In accordance with a first aspect of the invention, a detection apparatus for detecting charged particles is provided. The apparatus comprises a charged particle beam inlet. The apparatus further comprises a detection front or area comprising the entry face of at least one microchannel plate, MCP, assembly, wherein the entry face extends along a first direction (Z), wherein the MCP assembly is configured for receiving a beam of charged particles that impinge on its entry face and for generating, for each impinging charged particle, a corresponding amplified detection signal on its opposite exit face. The apparatus comprises at least one read-out anode for collecting said amplified detection signals, the anode being arranged at a distance to, and in parallel with the exit face of said at least one MCP assembly. Still further, the apparatus comprises beam deflection means arranged downstream of said inlet at a distance from said entry face and configured for selectively deflecting an incoming beam of charged particles along said first direction (Z), so that the corresponding charged particles selectively reach different portions of the MCP assembly's entry face along said first direction (Z).
In accordance with a another aspect of the invention, a detection apparatus for detecting charged particles is proposed. The apparatus comprises a charged particle beam inlet, a detection front comprising the entry face of at least one microchannel plate, MCP, assembly. The entry face extends along a first direction (Z). The MCP assembly is configured for receiving, along a second direction (X) perpendicular to said first direction, a plurality of beams of charged particles (10) that impinge on its entry face and for generating, for each impinging charged particle, a corresponding amplified detection signal on its opposite exit face. The apparatus further comprises at least one read-out anode for collecting said amplified detection signals, the anode being arranged at a distance to, and in parallel with the exit face of said at least one MCP assembly. The apparatus further comprises beam deflection means arranged downstream of said inlet at a distance from said entry face and configured for selectively deflecting an incoming beams of charged particles along said first direction (Z), so that the corresponding charged particles selectively reach different portions of the MCP assembly's entry face along said first direction (Z). The charged particle inlet, the beam deflection means, the detection front and the read-out anode extend along said second direction (X).
Preferably, the beam deflection means may comprise a charged particle optics unit and a control unit, the control unit being configured to dynamically control a deflection angle to be applied to the charged particle beam's propagation direction by the charged particle optics unit. The control unit may preferably comprise a data processing unit and a memory element, the data processing unit being programmed by a software code so as to implement the desired functions.
Preferably, the beam deflection means may comprise a charged particle optics unit and a control unit, the control unit being configured to dynamically control an opening angle within which the charged particle beam's propagation direction is deflected by the charged particle optics unit. The control unit may preferably comprise a data processing unit and a memory element, the data processing unit being programmed by a software code so as to implement the desired functions.
Preferably, the charged particle optics unit may comprise a pair of deflection plates or a Bradbury Nielsen Grid. The pair of deflection plates may preferably define a charged particle beam passage in between themselves.
The entry face of said at least one MCP assembly may preferably extend over 2 to 3 cm along said first direction (Z)
Preferably, the detection front or area may further extend along a second direction (X) perpendicular to said first direction (Z), and wherein entry faces of a plurality of MCP assemblies extend over an aggregated length of at least 15 cm in said second direction (X). The first direction may preferably be perpendicular to the plane in which the incoming charged particle beam's trajectory evolves prior to being deflected by said beam deflection means.
The entry faces of the plurality MCP assemblies may preferably extend over an aggregated length between 1 and 100 cm.
It may be preferred that a gap of at most 1 mm width separates the respective exit faces of any two adjacent MCP assemblies along said second direction (X).
The gap size between any two adjacent MCP assemblies may preferably be the same.
Preferably, the gap separating any two adjacent read-out anodes may have substantially the same width as the gap separating the entry and exit faces of the corresponding two adjacent MCP assemblies.
All MCP assemblies may preferably have substantially the same channel size and amplification gain characteristics.
Preferably, all MCP assemblies may have the same width extending perpendicularly to said principal direction.
The detector's front area may preferably consist of the entry faces of said MCP assemblies.
Preferably, the device may comprise biasing means configured for applying an electric potential difference between the respective entry and exit faces of each MCP assembly. The biasing means may preferably comprise a source of electricity.
The biasing means may preferably be configured for applying a positive or negative floating electric potential to the detector's front face. The biasing means may preferably comprise a source of electricity.
Preferably, the biasing means may be configured for applying a common electric potential to the respective exit faces of all MCP assemblies.
Preferably, the biasing means may be configured for applying a positive or negative floating electric potential to the beam deflection means. The potential may preferably be the same as the floating potential applied to the detector's front face.
Preferably the biasing means may be configured for applying a positive or negative floating electric potential to components of the apparatus. The components may preferably include the beam deflection means and the detector front, being part of the MCP assemblies.
The MCP assemblies may preferably comprise a stacked assembly of a plurality of multiple MCP devices, a chevron assembly or a Z-stacked assembly.
The apparatus may further preferably comprise one dedicated read-out anode for each MCP assembly, and said read-out anode may preferably extend along a corresponding MCP assembly's exit face.
The at least one read-out anode may preferably comprise a delay-line anode, a pixelated anode array, a resistive anode, a shaped anode, a single anode or any combination thereof.
Preferably, the beam deflection means may extend along said second direction (X).
Preferably, said charged particles may comprise ions. Preferably, the charged particles may comprise electrons.
In accordance with another aspect of the invention, a mass spectrometer for dispersing ions along a focal plane in accordance with their mass/charge ratio is provided. The spectrometer comprises a detection apparatus having a detection front, the detection front being arranged on said focal plane so that said dispersed ions impinge on the detection front. The spectrometer is remarkable in that said detection apparatus conforms to an aspect of the invention, and in that said first direction (Z), along which the detection front extends, is perpendicular to the plane in which the ions are dispersed by the mass spectrometer.
Preferably, deflection means of said detection apparatus comprised in said mass spectrometer may be are arranged so as to deflect all dispersed ions exiting a mass filtering unit of the mass spectrometer. The mass filtering unit may preferably comprise a magnetic sector instrument.
Preferably, the detection front of said detection apparatus comprised in said mass spectrometer may span said focal plane so that any ions dispersed by a mass filtering unit of the mass spectrometer impinge there upon.
Preferably, the mass spectrometer may be a Secondary Ion Mass Spectrometry, SIMS, device. The mass spectrometer device may further preferably be a Mattauch-Herzog type device.
The mass spectrometer may preferably be configured for being used in a floating configuration.
In accordance with a further aspect of the invention, a method for detecting charged particles is provided. The method uses the apparatus in accordance with an aspect of the invention. The method comprises the following steps:
In accordance with a further aspect of the invention, a method for detecting charged particles is provided. The method uses the apparatus in accordance with an aspect of the invention. The method comprises the following steps:
i′) providing a plurality of charged particle beams; the beams may preferably have a propagation direction;
ii′) using the device's beam deflection means, deflecting said charged particle beams in accordance with a predetermined deflection angle along said first direction (Z) in which at least one MCP assembly extends;
iii′) using the device's at least one read-out anode, reading out the amplified detection signals, as provided by said at least one MCP assembly;
iv′) repeating steps ii) and iii) at least once using a different predetermined detection angle.
In accordance with another aspect of the invention, a method of using the mass spectrometer in accordance with an aspect of the invention is provided. The method comprises the following steps:
Preferably, steps ii) and iii) or respectively b) and c) may be repeated so as to scan the charged particle beam or respectively the plurality of ion beams over the extent of the entry face of said at least one MCP assembly along said first direction (Z).
Preferably, steps ii) and iii) may be repeated so as to scan the extent of the entry face of said at least one MCP assembly along said first direction (Z).
Preferably, steps b) and c) may be repeated so as to scan the plurality of ion beams over the extent of the entry face of said at least one MCP assembly along said first direction (Z).
Preferably, the beam deflection means may comprise a charged particle optics unit and a control unit, the control unit being configured to dynamically control a deflection angle to be applied to the charged particle beam's propagation direction by the charged particle optics unit. Between two successive iterations of step ii) or respectively step b), the deflection angle may preferably be altered so that the spot generated during a first iteration by a deflected beam on the entry face of said at least one MCP assembly does not overlap with the spot generated during a second iteration by the same deflected beam.
Between two successive iterations of step ii), the deflection angle may preferably be altered so that the spot generated during a first iteration by the deflected beam on the entry face of said at least one MCP assembly does not overlap with the spot generated during a second iteration.
Between two successive iterations of step b), the deflection angle may preferably be altered so that the spot generated during a first iteration by a deflected ion beam on the entry face of said at least one MCP assembly does not overlap with the spot generated during a second iteration by the same deflected ion beam.
The successively read-out amplified detection signals may preferably be stored in a memory element and combined by a data processing unit so as to yield a combined detection signal corresponding to a given charged particle or to a given plurality of dispersed ion species.
The successively read-out amplified detection signals may preferably be stored in a memory element and combined by a data processing unit so as to yield a combined detection signal corresponding to a given charged particle.
Said combination may preferably comprise adding up successively read-out detection counts for a given charged particle.
The successively read-out amplified detection signals may preferably be stored in a memory element and combined by a data processing unit so as to yield a combined detection signal corresponding to a given plurality of dispersed ion species. The combined detection signal may preferably correspond to a mass spectrum data recorded using a given deflection angle.
The proposed invention provides a charged particle detection apparatus, which yields improved performance over known MCP-based charged particle detectors. To overcome the limitations of known MCP-based charged particle detectors, it is proposed to decouple the detectable ion beam signal from the detector's spatial resolution. In accordance with aspects of the invention, the number of the MCP channels of the detector that are involved in detecting a charged particle beam hitting the detector is increased. This is achieved by changing the position of the ion beam spot that hits the detector's front surface, where the MCP channel inlets are located. While a given set of MCP channels is saturated by the incoming beam, the beam is deflected to a set of yet unused MCP channels. The corresponding detection signals stemming from a plurality of sequentially sets of MCP-channels may be combined to reconstruct the total detection signal. While maintaining the detector's spatial resolution, the aspects of the proposed invention improve on the detectable maximum local count rate and dynamic range. An improvement factor of at least 10 has been observed. The proposed detection apparatus is particularly useful in a MCP-based 1D focal plane detector for high dynamic mass spectrometry applications, including Secondary Ion Mass Spectrometry, SIMS. In such a scenario, ion beams exiting the mass spectrometer's mass filtering unit (e.g. a magnetic sector instrument), are scanned in the vertical direction of the detector while not disturbing the spread of the focused ion beams in the horizontal direction.
Several embodiments of the present invention are illustrated by way of figures, which do not limit the scope of the invention, wherein:
This section describes features of the invention in further detail based on preferred embodiments and on the figures, without limiting the invention to the described embodiments. Unless otherwise stated, features described in the context of a specific embodiment may be combined with additional features of other described embodiments. Throughout the description, similar reference numerals will be used for similar or the same concept across different embodiments of the invention. For example, references 100, 200, 300, 400 and 500 each describe a detection apparatus in accordance with the invention, but in two respective embodiments thereof.
The description puts focus on those aspects of the proposed detector apparatus that are relevant for understanding the invention. It will be clear to the skilled person that the device also comprises other commonly known aspects, such as for example an appropriately dimensioned power supply, or a mechanical holder frame for holding the various elements of the apparatus in their respectively required positions, even if those aspects are not explicitly mentioned.
If the ion beam 10, 10′, 10″ is scanned along the Z-direction (see the dotted and dashed lines in
If the detection front is composed of a plurality of MCP assemblies along the X axis, all MCP assemblies may preferably have substantially the same channel size and amplification gain characteristics. Further, all MCP assemblies may have the same width extending perpendicularly to said principal direction, i.e. along the Z axis. The apparatus further comprises non-illustrated biasing means configured for applying an electric potential difference between the respective entry and exit faces of each MCP assembly. The biasing means may for example comprise a source of electricity. In accordance with a preferred embodiment of the invention, the biasing means are configured for applying a positive or negative floating electric potential to the detector's front face, and for applying a common electric potential to the respective exit faces of all MCP assemblies.
In accordance with a preferred embodiment of the invention, the deflection means of the proposed detection apparatus are provided by a device comprising deflection plates, as illustrated in
The two plates 332 in an ion beam deflector extend in parallel and define a passageway or gap for the charged particle beam 10 in between themselves. The deflector plates 332 are biased to opposite polarities to deflect the ion beams in a direction that is perpendicular to the plane in which the deflector plates extend. To this end, a source of electricity, voltage biasing unit or control unit 340 is used. The dimensions, relative arrangement and biasing electric potentials of the deflector 332, 334 are in practice optimised, for example through numerical simulation, to best match a given target application. By way of non-limiting example, the deflection plate width along the Y direction is preferably in the range from 2 mm to 8 mm. The distance between the plates 332 along the Z direction is preferably in the range from 3 mm to 5 mm. The gap between the plates 332 and the outer electrodes 334 (on both sides of the deflector to confine the fringe field regions to smaller distances) is in the range from 1 mm to 4 mm. Preferably, the distance between the plates is of about 4 mm, the gap between the plates and the outer electrodes is of about 2 mm, while the width of the plates along the Y direction is of about 6 mm. The distance between the outer electrodes, defining the inlet 302 of the apparatus, if preferably of about 6 mm. Preferably, the deflection plates 332 and outer electrodes 334 extend along the X axis, which is perpendicular to both Y and Z axes, by about 100 mm to 150 mm, and preferably by about 130 mm. Generally, the deflection length of the ion beams along the Z axis, i.e. the maximum span than can be scanned on the MCP assembly's entry face, increases with increasing deflection plate width. The mass resolution and transmission values decrease with increasing transmission plate width. The target of the deflection of 20 mm can be achievable for various combinations of the geometric and voltage values with the constraints of the mass resolution (at least up to half of the mass resolution observed at 0 V) and transmission (70%).
The working principle of the charged particle deflector 300 is as follows: the deflection distance along the Z axis, D, depends on the distance d between the deflection plates 332, their length L and the electrical potential difference (ΔV) that is applied to the pair of plates (±V). When an ion enters with an energy of eV0 into the electric field created between the two plates, (E=−ΔV/d) it will be deflected with a deflection angle θ.
Each MCP channel of an MCP assembly, whether of a single MCP, Chevron or Z-stack assembly, is characterized by recovery time, during which the channel cannot amplify a newly impinging charged particle. After a given response time, a saturated channel becomes once operational again. In accordance with a preferred embodiment, a control unit of the deflection means is therefore synchronized with the response time of the MCP assembly's micro-channels. The control unit effectively aims at steering the charged particle beam at all times, through deflection as previously described, to areas of the detection front that comprise operational MCP channels at the time of deflection. The speed of a continuously and linearly evolving scanning pattern is therefore preferably synchronized with the response time of the MCP channels, so that the charged particle beam illuminates the same channel only once it has completely recharged from the depletion caused by its previous illumination.
In an alternate embodiment, the control unit uses a sawtooth signal to scan multiple charged particle beams that are initially scattered along the X direction, periodically along the Z direction of the MCP assembly's detection front. A low-power high voltage operational amplifier scans the voltage of the ion deflection plates with a scan rate in the range from 1 Hz to 10 kHz. The scanning signal (sawtooth signal) consists of a combination of multiple scans of step voltages. The number of voltage steps depends on the size of the ion beams and the required deflection length of the ion beams in the vertical axis (Z) of the detector. A higher signal rate (>1 kHz) is desirable to achieve an enhanced signal count rate of the detector. The scanning rate is established in practice as a function of the recuperation time of a saturated channel of the MCP assembly When a measurement starts, the control unit sends a scanning signal to the high-voltage amplifier, and synchronously starts/triggers a Time-to-digital converter, TDC. Each time the step voltage changes, a pulse will pass to the TDC on a second line to increase an internal counter. During the acquisition, data is collected from the TDC. The raw data has acquired by the read-out anode and TDC has a format of {x position, y position, number of the voltage step, and iteration of the scan}. After multiple scans, there may be an integration time on each mass spectrum at different step voltages to combine all the mass spectra.
The deflection means 430 of the proposed detection apparatus comprise a Bradbury-Nielsen Gate, BNG, device. A BNG device consists of two interleaved sets of wires or strips 433, 434 extending along the Y direction, which are equally spaced and are biased at opposite polarities so that the deflecting field region is limited to short distances, typically twice of the diameter of the wires or length of the strips. The strip width is for example in the range from 0 to 1.6 mm, each strip having a thickness of 50-100 μm. The distance between the strips is in the range from 0.4 mm to 1 mm. By way of example, for a charged particle beam comprising ions at 3 keV, the voltage on the strips may be ramped from 0V up to ±800 V by a corresponding non-illustrated control unit of the deflection means. The deflection length of the ion beams increases with increasing strip width. The transmission values decrease with increasing strip width. Depending on the applied voltages, the BNG scatters charged particle beams within an angle having a voltage-dependent opening along the Z direction.
In all presented embodiments, the detector device is able to be floated to a high voltage of up to 10 kV, while the floating potential may have either positive or negative polarity. The floating potential may preferably be applied to all components of the detection apparatus, including the beam deflection means.
The N voltage/deflection steps are predetermined so that the correspondingly deflected spots generated by the deflected beam on the MCP entry faces span most of the entry face along the Z direction. Further, the response time of the MCP channels is taken into account: a given voltage step is applied during a time that corresponds at most to the time during which the MCP channels are capable of detection charged particles, until they saturate. Then the next voltage step is applied, wherein the difference between two steps is such that the deflected beam next illuminates a different set of micro-channels, which that are not in saturated mode. These measures maximize the availability of MCP channels for accurately counting detection events, thereby increasing the count rate of the apparatus. The corresponding calibration data depends on the type of MCP assembly that is used, on the dimensions of the apparatus, and on other factors. These data are provided on assembly of the apparatus and made available in a memory element to which the control unit 540 has read access.
At each of the N deflection steps, a corresponding detection signal is recorded using the read-out anode. Mass spectrum data for all m/z ratios is therefore recorded at each deflection step. The data corresponding to all steps is then combined, for example by adding up the successively read-out ion detection counts, to generate a full mass spectrum.
It should be understood that the detailed description of specific preferred embodiments is given by way of illustration only, since various changes and modifications within the scope of the invention will be apparent to the skilled person. The scope of protection is defined by the following set of claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| LU101794 | May 2020 | LU | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/EP2021/063007 | 5/17/2021 | WO |
