Abstract: A mass analyser for use in a mass spectrometer, the mass analyser having: a set of sector electrodes spatially arranged to provide an electrostatic field in a 2D reference plane suitable for guiding ions along an orbit in the 2D reference plane, wherein the set of sector electrodes extend along a drift path that is locally orthogonal to the reference plane so that, in use, the set of sector electrodes provide a 3D electrostatic field region; and an injection interface configured to inject ions into the mass analyser via an injection opening such that the ions injected into the mass analyser are guided by the 3D electrostatic field region along a 3D reference trajectory according to which ions perform multiple turns within the mass analyser whilst drifting along the drift path, wherein each turn corresponds to a completed orbit in the 2D reference plane.

Abstract: A mass spectrometer (1) includes: an ionization section (201) configured to generate ions from a sample; a mass separation section (231, 235) configured to separate ions generated by the ionization section according to mass-to-charge ratio; an ion detector (237) configured to detect an ion separated by the mass separation section; an ion capture section (31) configured to capture ions separated by the mass separation section; and an electron beam detection section (32) configured to detect an electron beam diffracted by ions captured within the ion capture section (31). This mass spectrometer is capable of performing, in a single measurement operation, both a mass spectrometric analysis and an electron-beam diffraction measurement for distinguishing between isomers. The electron-beam diffraction measurement can be more efficiently performed than in a conventional device of this type.

Abstract: A method of encoding a parent or precursor ion beam to aid product ion assignment is disclosed. According to an embodiment the energy of parent ions entering a collision cell 3 is progressively increased. Different species of parent ions fragment at different collision energies. Fragment ion intensity profiles are matched with parent ion intensity profiles to correlate fragment ions with corresponding parent ions.

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 ? 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. ?=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 ?2 and what is most important, compensating for mechanical misalignments of the optical components.

Abstract: In one aspect, a mass analyzer is disclosed, which comprises a quadrupole having an input end for receiving ions and an output end through which ions can exit the quadrupole, said quadrupole having a plurality of rods to at least some of which an RF voltage can be applied for generating a quadrupolar field for causing radial confinement of the ions as they propagate through the quadrupole and further generating fringing fields in proximity of said output end. The mass analyzer further includes at least a voltage source for applying a voltage pulse to at least one of said rods so as to excite radial oscillations of at least a portion of the ions passing through the quadrupole at secular frequencies thereof, where the radially-excited ions interact with the fringing fields as they exit the quadrupole such that their radial oscillations are converted into axial oscillations.

Abstract: A method of identifying and/or characterising ions comprises separating analyte ions according to a first physico-chemical property (ion-mobility), selecting first ions of the analyte ions, and activating, fragmenting or reacting the first ions to produce first product ions, separating the first product ions according to the first physico-chemical property, and determining a pattern of the first product ions. The first ions are identified and/or characterised using the pattern of the first product ions.

Abstract: An exemplary breath analysis system may include a sampling chamber having a molecule collector disposed therein. The molecule collector may be configured such that volatile organic compounds (VOCs) present in a breath sample introduced to the sampling chamber adhere to the molecule collector. A heating element may ramp heat within the sampling chamber, causing release of at least a portion of the VOCs adhered to the molecule collector, lighter and/or less bound VOCs first, heavier and/or more strongly bound VOCs later. An analysis device (e.g., a mass spectrometer or a Terahertz (THz) spectrometer) may identify one or more target VOCs from among at least the portion of the VOCs released from the molecule collector and generate an output representative of the identified target VOC(s). The output may include information that quantitates a concentration of the target VOC(s) with respect to a source of the breath sample.

Abstract: Techniques for simultaneous time-of-flight (ToF) measurement and information signal transmission. An information signal is superimposed on a series of light pulses by emitting the series of light pulses in groups of N regularly-spaced pulses and selectively varying time intervals between successive groups of pulses, such that the resulting varying time intervals between successive groups of emitted pulses are indicative of values of the information signal. Pixels configured to demodulate received light using a pulsed reference signal derived from the modulating signal are controlled to generate pixel signal values, each being indicative of a time-of-flight from the ToF measurement device to an object and back. This controlling comprises varying time intervals between successive groups of reference signal pulses in the same way time intervals between the emitted pulses are varied, so that the superimposition of the information signal has no effect on the ToF measurements.

Abstract: An exemplary breath analysis system may include a sampling chamber having a molecule collector disposed therein. The molecule detector may be configured such that volatile organic compounds (VOCs) present in a breath sample introduced to the sampling chamber adhere to the molecule collector. A heating element may introduce heat within the sampling chamber, causing release of at least a portion of the VOCs adhered to the molecule collector. An analysis device (e.g., a mass spectrometer or Terahertz (THz) spectrometer) may identify one or more target VOCs from among at least the portion of the VOCs released from the molecule collector and generate an output representative of the identified one or more target VOCs. The output may include information that quantitates a concentration of the one or more target VOCs with respect to a source of the breath sample.

Abstract: A method of proteolyzing a protein, including immobilizing a protein in at least one pore of a porous body, and contacting the protein immobilized in the pore and a protease immobilized on a solid surface such that the protease selectively accesses a site of the protein and proteolyzes the protein at the site.

Abstract: An instrument for separating ions may include an ion source configured to generate ions from a sample, at least one ion separation instrument configured to separate the generated ions as a function of at least one molecular characteristic and an electrostatic linear ion trap (ELIT) positioned to receive ions exiting the at least one ion separation instrument. The ELIT has first and second ion mirrors separated by a charge detection cylinder, and is configured such that an ion trapped therein oscillates back and forth through the charge detection cylinder between the first and second ion mirrors with a duty cycle, corresponding to a ratio of time spent by the trapped ion traversing the charge detection cylinder and total time spent by the trapped ion traversing a combination of the first and second ion mirrors and the charge detection cylinder during one complete oscillation cycle, of approximately 50%.

Abstract: Methods for an instrument including a light source of are provided. A method for an instrument including a light source includes providing light from the light source to a target location in a process chamber. The method includes receiving the light at a sensor. The method includes determining, using data from the sensor, a first position of the light at the target location. Moreover, the method includes determining whether to adjust the light to a second position at the target location. Related instruments are also provided.

Abstract: In one implementation, a mobility-based ion separation system includes a first ion channel extending between a first end and a second end, and configured to receive an ion packet. The separation system includes a controller configured to apply a first voltage signal and a second voltage signal to a first plurality of electrodes adjacent to the first ion channel. The first plurality of electrodes are configured to generate, based on receipt of the first voltage signal, a first traveling drive potential that travels at a first speed along a first direction, the first direction extending from the first end to the second end. The first plurality of electrodes are configured to generate, based on receipt of the second voltage signal, a second DC potential decreasing along a second direction, the second direction extending from the second end to the first end.

Abstract: We describe a method and apparatus for detecting humidity using a Field Asymmetric Ion Mobility Spectrometry (FAIMS) system. The system may comprise an ionizer for generating ions within a gas sample, wherein each ion has an associated ion mobility; an ion filter for separating the ions by applying a compensation field and a dispersion field to the generated ions; a detector for detecting an output from the ion filter; and a processor.

Abstract: An apparatus may include a first beam sensor, disposed adjacent a first position along a beamline. The apparatus may further include a second beam sensor, disposed adjacent a second position along the beamline, at a predetermined distance, downstream of the first beam sensor. The apparatus may include a detection system, coupled to the first beam sensor and to the second beam sensor to receive from a pulsed ion beam a first electrical signal from the first beam sensor and a second electrical signal from the second beam sensor.

Abstract: Atmospheric pressure ion guides are provided. The atmospheric pressure ion guides can include a multi-ring electrode structure connecting a larger opening to a smaller opening and having a series of ring electrodes with decreasing diameter and voltage going from the larger opening to the smaller opening. The electrodes can be made from stainless steel or other suitable conductive material. The multi-ring electrode structure can be contained in a housing, such as a housing made from polyetheretherketone or other suitable thermosetting polymer. The atmospheric pressure ion guide can focus ions from an ion source for use with ion detection devices such as an ion mobility spectrometer or a mass spectrometer. Methods of using the atmospheric pressure ion guides are provided, for example to focus a plurality of ions to be injected into an ion detection device. The atmospheric pressure ion guides can increase the signal intensity of the ion detection device.

Abstract: A system includes, an ion channel extending along a first direction from a first end to a second end. The ion channel is configured to receive ions at the first end of the ion channel. The system further includes a controller configured to apply a first voltage signal to a first plurality of electrodes adjacent to the ion channel. The first plurality of electrodes are configured to generate, based on receipt of the first voltage signal, a first traveling drive potential that travels along the first direction during a separation time. One or more of a travel speed and an amplitude of the first traveling drive potential vary during a first time segment of the separation time.

Abstract: The present invention relates to methods of improving analytical instruments and improved analytical instruments. The aforementioned method employs a calibration correction module that calibrates the machine to effect measurements with the minimum possible relative squared error. This results in a significant improvement of the analytical instrument in question that leads to more precise and accurate results.

Abstract: A method is disclosed comprising: trapping ions in an ion trap (40); applying a first force on the ions within the ion trap in a first direction, said force having a magnitude that is dependent upon the value of a physicochemical property of the ions; applying a second force on these ions in the opposite direction so that the ions separate according to the physicochemical property value as a result of the first and second forces; and then pulsing or driving ions out of one or more regions of the ion trap.

Abstract: A method of filtering ions according to their ion mobility using a device is disclosed, the method comprising a plurality of electrodes and one or more voltage source(s) arranged and adapted to apply voltages to the plurality of electrodes, the method comprising, generating using the one or more voltage source(s) one or more local separation region(s), wherein ions can be separated within each local separation region according to their ion mobility, and moving each local separation region axially along the device with a certain velocity such that, for each local separation region, ions having a value of their ion mobility falling within a selected range are transmitted axially along the device with that local separation region whereas ions having higher and/or lower ion mobility falling outside that range escape the local separation region, wherein any ions that escape the local separation region(s) are removed from within the device and/or otherwise kept apart from those ions falling within the selected rang

Abstract: An ion mirror 41 constructed of thin electrodes that are interconnected by resistive dividers 45 with potentials U1-U5 applied to knot electrodes to form segments 41-43 of linear potential distribution between the “knot” electrodes, yet without separating those field regions by meshes. Weak and controlled penetration of electric fields provide for a fine control over the field non linearity and over the equipotential line curvature, thus allowing to reach unprecedented level of ion optical quality: more than twice larger energy acceptance compared to thick electrode mirrors, up to sixth order time per energy focusing, ion spatial focusing and wide spatial acceptance. Novel mirrors can be formed very slim to arrange them into stacks for ion transverse displacement between ion reflections or for multiplexed mirror stacks. Printed circuit boards (PCB) are best suited for making novel ion mirrors, while novel ion mirrors are designed to suit PCB requirements.

Abstract: Inside a chamber (10) evacuated by a vacuum pump, a flight tube (12) is held via a support member (11) that is of insulation. The outside of the chamber (10) is surrounded by a temperature control unit (16) including a heater. A body (10a) of the chamber (10) is made of aluminum, and a coating layer (10b) by a black nickel plating is formed on the inner wall surface of the body (10a) of the chamber (10). Due to this, the radiation factor of the chamber (10) becomes higher than that of a conventional apparatus using only aluminum, and the thermal resistance of the radiation heat transfer path between the chamber (10) and the flight tube (12) becomes low, thus improving the temperature stability of the flight tube (12). Furthermore, the time constant of the temperature change of the flight tube (12) becomes small, thus reducing the time for the flight tube (12) to stabilize to a constant temperature.

Abstract: Embodiments of systems, devices, and methods relate to an electrode standoff isolator. An example electrode standoff isolator includes a plurality of adjacent insulative segments positioned between a proximal end and a distal end of the electrode standoff isolator. A geometry of the adjacent insulative is configured to guard a surface area of the electrode standoff isolator against deposition of a conductive layer of gaseous phase materials from a filament of an ion source.

Abstract: A method for analyzing particles in an air stream includes concentrating the particles in an interior region of the air stream and deflecting the concentrated particles in the air stream with a generated thermal gradient. Smaller particles in the air stream may be selectively deflected away from the interior region and towards a periphery of the air stream at a different rate than larger particles in the air stream. The generated thermal gradient may be controlled to deflect particles in a selected particle size range onto a surface of a particle detector. An effective mass of the collected particles and an aerosol mass concentration estimate of the particles within the selected particle size range may be generated. Systems for analyzing particles are also disclosed.

Abstract: An example system includes an ion detector and a signal processing apparatus in communication with the ion detector. The ion detector is arranged to detect ions during operation of the system and to generate a signal pulse in response to the detection of an ion. The signal pulse has a peak amplitude related to at least one operational parameter of the system. The signal processing apparatus is configured to analyze signal pulses from the ion detector and determine information about the detected ions during operation of the system based on the signal pulses. The signal processing apparatus includes a discriminator circuit. The signal processing apparatus is programmed to vary a threshold of the discriminator circuit based on the at least one operational parameter of the system during operation of the system.

Abstract: A no-electric field region (246A) and an electric field region (246B) are formed in a flight tube (246). In the no-electric field region (246A), ions introduced from an ion emission unit fly. In the electric field region (246B), a reflectron (244) is provided and the ions having passed through the no-electric field region (246A) are reflected to the no-electric field region (246A) by an action of an electric field formed on an inner side of a plurality of electrodes (244A, 244B). A through-hole (246D) is formed in at least a part of the flight tube (246) to be closer to the electric field region (246B) than the no-electric field region (246A).

Abstract: The invention relates to an ion mobility spectrometer which has at least a first drift chamber and a first switchable ion gate for the controlled transfer of ions into the first drift chamber, wherein:—the first ion gate is designed as a field switching ion gate having at least a first counter electrode and a first injection electrode; wherein—a first ionization chamber is formed between the first counter electrode and the first injection electrode, into which first ionization chamber ions to be analyzed by ion mobility spectrometry can be fed from an ionization source. The invention also relates to an ion mobility spectrometer which has at least a first drift chamber and a first switchable ion gate for the controlled transfer of ions into the first drift chamber and a second drift chamber separated from the first drift chamber and a second switchable ion gate for the controlled transfer of ions into the second drift chamber.

Abstract: On field ionization under ambient conditions is described and applied on both ionization and desorption of various chemicals and biochemical present on the surface of materials in solid, liquid or gas states. The Atmospheric Pressure Megavolt Electrostatic Field Ionization Desorption (APME-FID) method generates ions directly from the surface of samples connected to a high electrical voltage at megavolt conditions. Megavolt electrostatic potential is generated and gradually accumulated directly on the sample surface by a Van de Graaff generator without causing damage to the sample. Therefore, when coupled with mass spectrometric system, the APME-FID-MS method enables direct detection of analytes on the surface of samples in different sizes and diverse types.

Abstract: A quadrupole mass spectrometer includes an ion source that ionizes a sample, a filter unit that includes a quadrupole and separates ions generated from the ion source according to mass, a detector that detects ions passing through the filter unit, a filter voltage controller that controls a filter voltage applied to the quadrupole to switch between a blocking mode in which ions entering the filter unit are not allowed to impinge on the detector and a passing mode in which ions entering the filter unit are allowed to impinge on the detector, the filter voltage including a radio-frequency voltage and a direct-current voltage, a baseline computing unit that computes a baseline based on outputs of the detector in the blocking mode, and an analyzing unit that outputs an analysis result of the sample based on outputs of the detector in the passing mode and the computed baseline.

Abstract: An analytical device includes: a mass spectrometry unit that separates ions based on flight time and detects the ions having been separated; an analysis unit that creates data corresponding to a spectrum in which an intensity of the ions having been detected and the flight time or m/z corresponding to the flight time are associated; a peak width calculation unit that calculates a first peak width at a first intensity and a second peak width at a second intensity different from the first intensity for at least one peak in the spectrum; and an adjustment unit that performs an adjustment of the mass spectrometry unit based on the first peak width and the second peak width.

Abstract: Improved multi-pass time-of-flight mass spectrometers MPTOF, either multi-reflecting (MR) or multi-turn (MT) TOF are proposed with elongated pulsed converters—either orthogonal accelerator or radially ejecting ion trap. The converter (35) is displaced from the MPTOF s-surface of isochronous ion motion in the orthogonal Y-direction. Long ion packets (38) are pulsed deflected in the transverse Y-direction and brought onto said isochronous trajectory s-surface, this way bypassing said converter. Ion packets are isochronously focused in the drift Z-direction within or immediately after the accelerator, either by isochronous trans-axial lens/wedge (68) or Fresnel lens. The accelerator is improved by the ion beam confinement within an RF quadrupolar field or within spatially alternated DC quadrupolar field. The accelerator improves the duty cycle and/or space charge capacity of MPTOF by an order of magnitude.

Abstract: An improved multi-pass time-of-flight or electrostatic trap mass spectrometer (70) with an orthogonal accelerator, applicable to mirror based multi-reflecting (MR) or multi-turn (MT) analyzers. The orthogonal accelerator (64) is tilted and after first ion reflection or turn the ion packets are back deflected with a compensated deflector (40) by the same angle ? to compensate for the time-front steering and for the chromatic angular spreads. The focal distance of deflector (40) is control by Matsuda plates or other means for producing quadrupolar field in the deflector. Interference with the detector rim is improved with dual deflector (68). The proposed improvements allow substantial extension of flight path and number of ion turns or reflections. The problems of analyzer angular misalignments by tilting of ion mirror (71) is compensated by electrical adjustments of ion beam (63) energy and deflection angles in deflectors (40) and (68).

Abstract: To acquire a mass spectrum for a wide mass range, a normal analysis execution controlling unit controls components to repeatedly perform measurement while changing setting m/z by a predetermined m/z at a time, and a mass spectrum summarizing processing unit summarizes data pieces each obtained by each time of measurement to generate the mass spectrum. Radio-frequency voltage applied to an ion guide and the like is changed based on the setting m/z. The radio-frequency voltage for the setting m/z is determined using a table in which a relationship between a position on an axis between upper and lower limits of the mass range and the radio-frequency voltage is substantially the same regardless of the mass range.

Abstract: A composition formula of each precursor ion located on a measured mass spectrum is estimated from the m/z value of the precursor ion (S11). A composition formula of each product ion located on a measured MS/MS spectrum is estimated from the m/z value of the product ion (S11). For each product-ion peak, the assignment of the peak is determined by verifying consistency between the composition formula of the product ion and the composition formula of each of the precursor ions (S13-S14). Based on the assignment result, the MS/MS spectrum data are separated and an MS/MS spectrum for each precursor ion is created (S15-S16). In this manner, MS/MS spectra which respectively correspond to a plurality of compounds can be created from an MS/MS spectrum in which the product ions originating from those compounds are mixed, and those compounds can be identified.

Abstract: A time-to-digital converter obtains a Start signal to indicate the start of an event, and a Stop signal whose assertion indicates the stop of the event. The Stop signal can be asserted multiple times due to false indications of the event stop. The TDC continuously monitors the Stop signal to generate a separate digital value for the duration from the event's starting time to each assertion of the Stop signal. The digital values can be analyzed to select the true duration of the event. Other features and embodiments are also provided.

Abstract: A method for generating an optimum vertical trajectory of a flight trajectory of an aircraft in the descent/approach phase. The trajectory is defined between a current state and a target state of the aircraft on the basis of a speed profile of the aircraft as a function of a curvilinear abscissa of the aircraft along a flight plan. The profile corresponds to a transition between the current and target states and is broken down into successive segments each corresponding to a different aerodynamic configuration that the aircraft may adopt during the descent/approach phase. The method is based on defining a set of flight strategies, each strategy of the set being defined using for each segment of the speed profile flight parameters chosen randomly in ranges of values compatible with the aerodynamic configuration corresponding to that segment. Optimum vertical trajectory is generated on the basis of the strategy of the set.

Abstract: The disclosure features methods and systems that include directing an ion beam to a region of a sample to liberate charged particles from the region of the sample, where the directed ion beam is pulsed at a first repetition rate, deflecting a first subset of the liberated charged particles from a first path to a second path different from the first path in response to a gate signal synchronized with the repetition rate of the pulsed ion beam, and detecting the first subset of the liberated charged particles in a time-of-flight (TOF) mass spectrometer to determine information about the sample, where the gate signal sets a common reference time for the TOF mass spectrometer for the first subset of charged particles liberated by each pulse of the ion beam.

Abstract: A multi-reflecting time-of-flight mass spectrometer MR TOF with an orthogonal accelerator (40) is improved with at least one deflector (30) and/or (30R) in combination with at least one wedge field (46) for denser folding of ion rays (73). Systematic mechanical misalignments (72) of ion mirrors (71) may be compensated by electrical tuning of the instrument, as shown by resolution improvements between simulated peaks for non compensated case (74) and compensated one (75), and/or by an electronically controlled global electrostatic wedge/arc field within ion mirror (71).

Abstract: Inside a chamber (10) evacuated by a vacuum pump, a flight tube (12) is held via a support member (11) that is of insulation. The outside of the chamber (10) is surrounded by a temperature control unit (16) including a heater. A body (10a) of the chamber (10) is made of aluminum, and a coating layer (10b) by a black nickel plating is formed on the inner wall surface of the body (10a) of the chamber (10). Due to this, the radiation factor of the chamber (10) becomes higher than that of a conventional apparatus using only aluminum, and the thermal resistance of the radiation heat transfer path between the chamber (10) and the flight tube (12) becomes low, thus improving the temperature stability of the flight tube (12). Furthermore, the time constant of the temperature change of the flight tube (12) becomes small, thus reducing the time for the flight tube (12) to stabilize to a constant temperature.

Abstract: An apparatus for transporting charged particles. The apparatus includes a control unit and a transport device having a plurality of electrodes arranged around a transport channel, wherein the transport channel includes a bunch forming region configured to receive charged particles received by the transport device. The control unit is configured to control voltages applied to the electrodes to generate a transport potential in the transport channel, the transport potential having a plurality of potential wells which are configured to move so as to transport charged particles along the transport channel in one or more bunches.

Abstract: A multi-reflection mass spectrometer comprising two ion mirrors spaced apart and opposing each other in a direction X, each mirror elongated generally along a drift direction Y, the drift direction Y being orthogonal to the direction X, a pulsed ion injector for injecting pulses of ions into the space between the ion mirrors, the ions entering the space at a non-zero inclination angle to the X direction, the ions thereby forming an ion beam that follows a zigzag ion path having N reflections between the ion mirrors in the direction X whilst drifting along the drift direction Y, a detector for detecting ions after completing the same number N of reflections between the ion mirrors, and an ion focusing arrangement at least partly located between the opposing ion mirrors and configured to provide focusing of the ion beam in the drift direction Y, such that a spatial spread of the ion beam in the drift direction Y passes through a single minimum at or immediately after a reflection having a number between 0.

Abstract: An ion sensor, an ion sensor manufacturing method, and a field asymmetric ion mobility spectrometry (FAIMS) system. The ion sensor includes an ion filter including a first electrode and a second electrode facing each other, an ion sensing electrode with which an ion that has passed through the ion filter collides, and an insulator to electrically insulate the ion sensing electrode from the first electrode and the second electrode. The method includes forming a first slit on an active layer of an at least one SOI substrate, the at least one SOI substrate including a base layer, an insulating layer on the base layer, and the active layer on the insulating layer, dividing the active layer into two, forming a second slit through the base layer, the second slit overlapping with the first slit in a planar view, and forming a third slit through the insulating layer.

Abstract: To provide an ion detector having an electron lens structure that enables expansion of an effective region of an MCP for capturing ions. The ion detector comprises an MCP unit including an MCP and a first focus electrode, a signal output device including an electron detector surface, and a reset unit disposed between the MCP unit and the signal output device. The reset unit includes a reset element and a second focus electrode. The reset element includes a second input surface and a second output surface opposing each other. On the second output surface, the reset element resets variations in incident angle and velocity of electrons on the second input surface.

Abstract: An ion source of an ion trap mass spectrometer generates ions of a component in a sample. An ion trap captures the ions generated by the ion source. An ion detector detects ions ejected from the ion trap. A voltage application control part changes a voltage applied to the ion detector such that, after generation of ions by the ion source is started, ion detection capability of the ion detector during a time period when ions having a mass-to-charge ratio outside an analysis target range are ejected from the ion trap is lower as compared to ion detection capability of the ion detector during a time period when ions having a mass-to-charge ratio within the analysis target range are ejected from the ion trap.

Abstract: A fluid ejection and circulation apparatus may include a fluid ejection die, the pressure regulator, a first standpipe, a second standpipe and a crossflow passage. The pressure regulator has a fluid chamber. The first standpipe is between the fluid chamber and the fluid ejection die. The first standpipe has a first port above the fluid ejection die. The second standpipe extends alongside the first standpipe. The second standpipe has a second port above the fluid ejection die. The crossflow passage connects the first standpipe and the second standpipe.

Abstract: A method of calibrating or optimising an analytical instrument is disclosed that comprises analysing analyte from a sample using an analytical instrument, determining a sample type of the sample based on analysis of analyte from the sample, identifying one or more species of the analyte that are known to be endogenous to the determined sample type, and calibrating or optimising the analytical instrument using the one or more identified endogenous species.

Abstract: An IMS ionizer comprising a wire, a second conductor, and a dielectric, when the first conductor and second conductor are energized to an ionization voltage, discharge ionization occurs. The dielectric is a glass element formed in a tubular shape defining an inner wall. The wire is formed in coils in contact with said inner wall. The second conductor is positioned to define an outer wall of the tube. The tube has an inlet end for receiving the sample, and an outlet end through which the sample exits after ionization.

Abstract: The present invention can be directed to a mass spectrometer, relevant parts thereof like replacement kits or upgrading kits and/or mass spectrometry methods. A mass spectrometer according to the present invention can comprise at least one ion source for generating a beam of ions from a sample. Moreover at least one mass filter downstream of the ion source can be provided and adapted to select ions from the beam by their mass-to-charge ratio (m/z). Furthermore at least one collision cell arranged downstream of the mass filter can be arranged. At least one sector field mass analyser arranged downstream of the collision cell can be further provided and at least one ion multicollector comprising a plurality of ion detectors arranged downstream of the mass analyser, for detecting a plurality of different ion species in parallel and/or simultaneously.

Abstract: A method of ion mobility spectrometry is disclosed comprising: transmitting a plurality of ions to an ion mobility separator 6; modulating the introduction of the ions into the ion mobility separator 6 at a first modulation frequency; separating the ions that enter the ion mobility separator 6 according to ion mobility; detecting ions that have exited the ion mobility separator with a detector of a time of flight mass analyser 8; varying the first modulation frequency with time; recording the intensity of the ion signal output from the detector to produce recorded data; modulating the recorded data as a function of the time that the data was recorded and at a second modulation frequency, wherein the second modulation frequency is varied as a function of the time that the data was recorded; and determining, from the variation in intensity of the ion signal in the modulated data as a function of the second modulation frequency, the ion mobilities of the ions that have been detected.

Abstract: An approach for detecting a transient error in a body fluid sample based on the shape of a response curve of a sensor is provided. The response curve is represented by an equation including at least one coefficient describing a curvature or slope of the response curve. The approach includes comparing the coefficient to a range of coefficients which includes coefficients of response curves corresponding to known analyte concentrations. The approach further includes detecting a transient error based on the comparison. In some examples of the approach, the comparison and detection are performed by a processing transient error detector executing computer readable instructions embodied in a non-transitory computer-readable medium. Other examples of the approach determine a concentration of the analyte based on the equation. Advantageously, various examples of the approach can expedite detection of transient errors at the time of measuring and before reporting sample result.