THERMO FISHER SCIENTIFIC (BREMEN) GMBH Patent applications |
Patent application number | Title | Published |
20160141167 | Collision Cell - A method of operating a gas-filled collision cell in a mass spectrometer is provided. The collision cell has a longitudinal axis. Ions are caused to enter the collision cell. A trapping field is generated within the collision cell so as to trap the ions within a trapping volume of the collision cell, the trapping volume being defined by the trapping field and extending along the longitudinal axis. Trapped ions are processed in the collision cell and a DC potential gradient is provided, using an electrode arrangement, resulting in a non-zero electric field at all points along the axial length of the trapping volume so as to cause processed ions to exit the collision cell. The electric field along the axial length of the trapping volume has a standard deviation that is no greater than its mean value. | 05-19-2016 |
20160141164 | Method for Time-Alignment of Chromatography-Mass Spectrometry Data Sets - A method is disclosed for adjusting the time scale of chromatography-mass spectrometry data sets, wherein a time scale of a first data set is used as a reference time scale and wherein a time scale of at least one second data set is adapted to the reference time scale comprising the. The steps of the method include identifying feature groups in the first data set by evaluating intensities of consecutive points of the first data set; identifying feature groups in the second data set by evaluating intensities of consecutive points of the second data set; matching feature groups of the first data set to feature groups of the second data set, and determining a corrected time scale for the second data set based on time differences between feature groups in the first data set and matching feature groups in the second data set. | 05-19-2016 |
20160111267 | Ion Detection System and Method - A detection system and a method for detecting ions which have been separated in a time-of-flight (TOF) mass analyzer, comprising an amplifying arrangement for converting ions into packets of secondary particles and amplifying the packets of secondary particles, wherein the amplifying arrangement is arranged so that each packet of secondary particles produces at least a first output and a second output separated in time and so that during the delay between producing the first and second output the first output produced by a packet of secondary particles is used for modulating the second output produced by the same packet. An increased dynamic range of detection and protection of the detection system against intense ion pulses is thereby provided. | 04-21-2016 |
20160084799 | Apparatus and Methods for Ion Mobility Spectrometry - A method of ion mobility spectrometry wherein ions undergo multiple stages of ion mobility separation and multiple stages of inertial ion motion wherein the mean free path between ion collisions with gas is significantly longer than in the stages of ion mobility separation, wherein each stage of inertial ion motion lies between successive stages of ion mobility separation. | 03-24-2016 |
20160079052 | Method and Apparatus for Mass Spectrometry - A method for analysing ions according to their mass-to-charge ratio and mass spectrometer for performing the method, comprising directing a collimated ion beam along an ion path from an ion source to an ion detector, causing a portion of the ion beam to contact one or more surfaces prior to reaching the ion detector, wherein the method comprises providing a coating on and/or heating the one or more surfaces to reduce variation in their surface patch potentials. The method is applicable to multi-reflection time-of-flight (MR TOF) mass spectrometry. | 03-17-2016 |
20160027633 | Collision Cell Multipole - Mass spectrometer collision/reaction cell multipole and method. The multipole may have first and second portions and an intermediate portion therebetween, the first and second portions operating at first and second q values lower than a third q value at the intermediate portion. A low-mass cut-off of the multipole may be controlled by varying a q value from a first to at least a second value. The multipole may have multipole electrodes disposed about a central axis and having a respective first portion, second portion, and intermediate portion therebetween which is radially closer to the central axis. This offers relatively high acceptance and ion transmission, while providing low-mass cut-off for removing undesired/interfering ions and helping reduce background count. | 01-28-2016 |
20160005585 | MULTI-REFLECTION MASS SPECTROMETER - A multi-reflection mass spectrometer is provided comprising two ion-optical mirrors, each mirror elongated generally along a drift direction (Y), each mirror opposing the other in an X direction, the X direction being orthogonal to Y, characterized in that the mirrors are not a constant distance from each other in the X direction along at least a portion of their lengths in the drift direction. In use, ions are reflected from one opposing mirror to the other a plurality of times while drifting along the drift direction so as to follow a generally zigzag path within the mass spectrometer. The motion of ions along the drift direction is opposed by an electric field resulting from the non-constant distance of the mirrors from each other along at least a portion of their lengths in the drift direction that causes the ions to reverse their direction. | 01-07-2016 |
20160005580 | MULTI-REFLECTION MASS SPECTROMETER - A multi-reflection mass spectrometer comprising two ion-optical mirrors, each mirror elongated generally along a drift direction (Y), each mirror opposing the other in an X direction and having a space therebetween, the X direction being orthogonal to Y; the mass spectrometer further comprising one or more compensation electrodes each electrode being located in or adjacent the space extending between the opposing mirrors; the compensation electrodes being configured and electrically biased in use so as to produce, in at least a portion of the space extending between the mirrors, an electrical potential offset which: (i) varies as a function of the distance along the drift length, and/or; (ii) has a different extent in the X direction as a function of the distance along the drift length. In a preferred embodiment the period of ion oscillation between the mirrors is not substantially constant along the whole of the drift length. | 01-07-2016 |
20150364316 | Electrostatic Trap - An electrostatic trap such as an orbitrap is disclosed, with an electrode structure. An electrostatic trapping field of the form U′(r, φ, z) is generated to trap ions within the trap so that they undergo isochronous oscillations. The trapping field U′(r, φ, z) is the result of a perturbation W to an ideal field U(r, φ, z) which, for example, is hyperlogarithmic in the case of an orbitrap. The perturbation W may be introduced in various ways, such as by distorting the geometry of the trap so that it no longer follows an equipotential of the ideal field U(r, φ, z), or by adding a distortion field (either electric or magnetic). The magnitude of the perturbation is such that at least some of the trapped ions have an absolute phase spread of more than zero but less than 2 π radians over an ion detection period T | 12-17-2015 |
20150364308 | COLLISION CELL - A method of operating a gas-filled collision cell in a mass spectrometer is provided. The collision cell has a longitudinal axis. Ions are caused to enter the collision cell. A trapping field is generated within the collision cell so as to trap the ions within a trapping volume of the collision cell, the trapping volume being defined by the trapping field and extending along the longitudinal axis. Trapped ions are processed in the collision cell and a DC potential gradient is provided, using an electrode arrangement, resulting in a non-zero electric field at all points along the axial length of the trapping volume so as to cause processed ions to exit the collision cell. The electric field along the axial length of the trapping volume has a standard deviation that is no greater than its mean value. | 12-17-2015 |
20150357981 | Transimpedance Amplifier - A transimpedance amplifier includes a resistor assembly coupled between an output of the transimpedance amplifier and an input of the transimpedance amplifier, and a voltage source for applying a first voltage to a first conductive compensation element of the resistor assembly and a second voltage to a second conductive compensation element of the resistor assembly. The first voltage and the second voltage are each derived from the output voltage, V | 12-10-2015 |
20150348767 | Imaging Mass Spectrometry Method and Device - A method of performing imaging mass spectrometry of a sample. The method comprises performing a first mass analysis of the sample using a first mass analyzer comprising a multi-pixel ion detector to obtain first mass spectral data representative of pixels of the sample. The method further comprises identifying clusters of pixels sharing one or more characteristics of first mass spectral data. The method also comprises performing a second mass analysis of the sample using a second mass analyzer to obtain second mass spectral data at at least one location in each cluster, wherein the number of locations is significantly less than the number of pixels in each cluster, said second mass analysis being of higher resolution than said first mass analysis. Also a mass spectrometry apparatus configured for carrying out the method. | 12-03-2015 |
20150340217 | Targeted Analysis for Tandem Mass Spectrometry - A tandem mass spectrometer and method are described. Precursor ions are generated in an ion source and an ion injector injects ions towards a downstream ion guide via a single or multi reflection TOF device that separates ions into packets in accordance with their m/z. A single pass ion page in the path of the precursor ions between the ion injector and the ion guide is controlled so that (only a subset of precursor ion packets, containing precursor ions of interest, is allowed onward transmission to the ion guide. A high resolution mass spectrometer is provided for analysis of those ions, or their fragments, which have been allowed passage through the ion gate. The technique permits multiple m/z ranges to be selected from a wise mass range of precursors, with optional fragmentation of one or more of the chosen ion species. | 11-26-2015 |
20150340213 | Method and Apparatus for Mass Spectrometry of Macromolecular Complexes - A method of analyzing macromolecular complex ions, such protein complex ions, by mass spectrometry and apparatus for performing the method, wherein the method comprises: introducing macromolecular complex ions into a first fragmentation device and trapping the complex ions therein for a trapping period; fragmenting the trapped complex ions in the first fragmentation device to produce monomer subunit ions; optionally selecting one or more species of subunit ions by m/z; introducing one or more of the species of subunit ions into a second fragmentation device, spatially separated from the first fragmentation device; fragmenting the subunit ions in the second fragmentation device to produce a plurality of first fragment ions of the subunit ions; and mass analyzing the first fragment ions in a mass analyzer, or subjecting the first fragment ions to one or more further steps of fragmentation to form further fragment ions and mass analyzing the further fragment ions. | 11-26-2015 |
20150325424 | Method of Assessing Vacuum Conditions in a Mass Spectrometer - A method is proposed for assessing the vacuum conditions in a mass spectrometer ( | 11-12-2015 |
20150294849 | Multireflection Time-of-flight Mass Spectrometer - A method of reflecting ions in a multireflection time of flight mass spectrometer is disclosed. The method includes guiding ions toward an ion mirror having multiple electrodes, and applying a voltage to the ion mirror electrodes to create an electric field that causes the mean trajectory of the ions to intersect a plane of symmetry of the ion mirror and to exit the ion mirror, wherein the ion are spatially focussed by the mirror to a first location and temporally focused to a second location different from the first location. Apparatus for carrying out the method is also disclosed. | 10-15-2015 |
20150287583 | HIGH DUTY CYCLE ION SPECTROMETER - An ion spectrometer is provided, comprising: an ion source, arranged to generate ions continuously with a first range of mass to charge ratios; and an ion trap, arranged to receive ions from the ion source along an axis, and to eject ions with a second range of mass to charge ratios orthogonally to that axis, the second range of mass to charge ratios being narrower than the first range of mass to charge ratios. In some embodiments, ions generated by the ion source continuously flow into the ion trap. Additionally or alternatively, ion optics receive ions ejected from the ion trap and cool the ions without substantial fragmentation. An ion analyser receives ions ejected from the ion trap or ion optics and separates the ions in accordance with at least one characteristic of the ions. | 10-08-2015 |
20150279641 | Parallel Mass Analysis - A system and method of mass spectrometry is provided. Ions from an ion source are stored in a first ion storage device and in a second ion storage device. Ions are ejected from the first ion storage device to a first mass analysis device during a first ejection time period, for analysis during a first analysis time period. Ions are ejected from the second ion storage device to a second mass analysis device during a second ejection time period. The ion storage devices are connected in series such that an ion transport aperture of the first ion storage device is in communication with an ion transport aperture of the second ion storage device. The first analysis time period and the second ejection time period at least partly overlap. | 10-01-2015 |
20150228466 | Mass Spectrometer Vacuum Interface Method and Apparatus - A mass spectrometer vacuum interface can include a skimmer apparatus having a skimmer aperture and an internal surface. A method of operating the mass spectrometer vacuum interface can include establishing an outwardly directed flow along the internal surface of the skimmer apparatus. | 08-13-2015 |
20150155147 | Targeted Analysis for Tandem Mass Spectrometry - A tandem mass spectrometer and method are described. Precursor ions are generated in an ion source and an ion injector injects ions towards a downstream ion guide via a single or multi reflection TOF device that separates ions into packets in accordance with their m/z. A single pass ion page in the path of the precursor ions between the ion injector and the ion guide is controlled so that (only a subset of precursor ion packets, containing precursor ions of interest, is allowed onward transmission to the ion guide. A high resolution mass spectrometer is provided for analysis of those ions, or their fragments, which have been allowed passage through the ion gate. The technique permits multiple m/z ranges to be selected from a wise mass range of precursors, with optional fragmentation of one or more of the chosen ion species. | 06-04-2015 |
20150122989 | Electrostatic Trap - An electrostatic trap such as an orbitrap is disclosed, with an electrode structure. An electrostatic trapping field of the form U′(r, Φ, z) is generated to trap ions within the trap so that they undergo isochronous oscillations. The trapping field U′(r, Φ, z) is the result of a perturbation W to an ideal field U(r, Φ, z) which, for example, is hyperlogarithmic in the case of an orbitrap. The perturbation W may be introduced in various ways, such as by distorting the geometry of the trap so that it no longer follows an equipotential of the ideal field U(r, Φ, z), or by adding a distortion field (either electric or magnetic). The magnitude of the perturbation is such that at least some of the trapped ions have an absolute phase spread of more than zero but less than 2 π radians over an ion detection period T | 05-07-2015 |
20150102215 | Collision Cell Multipole - Mass spectrometer collision/reaction cell multipole and method. The multipole may have first and second portions and an intermediate portion therebetween, the first and second portions operating at first and second q values lower than a third q value at the intermediate portion. A low-mass cut-off of the multipole may be controlled by varying a q value from a first to at least a second value. The multipole may have multipole electrodes disposed about a central axis and having a respective first portion, second portion, and intermediate portion therebetween which is radially closer to the central axis. This offers relatively high acceptance and ion transmission, while providing low-mass cut-off for removing undesired/interfering ions and helping reduce background count. | 04-16-2015 |
20150056060 | Multiple Port Vacuum Pump System - A vacuum pump system for evacuating at least five volumes comprising a turbomolecular pump and a forevacuum pump arranged to pump an output of the turbomolecular pump arrangement to atmosphere. The turbomolecular pump has at least five pumping stages separated by rotor blades. Not more than three pumping stages have pumping speeds in excess of ⅓ of the highest pumping speed when under vacuum and/or a pumping port cross section in excess of ⅓ of the highest pumping port cross section, and at least two pumping stages have pumping speeds less than ¼ of the highest pumping speed when under vacuum and/or a pumping port cross section of less than ¼ of the biggest pumping port cross section. The ratio of pressures between the pumping stage with the highest pressure and the pumping stage with the lowest pressure is at least 100000:1 when under vacuum. | 02-26-2015 |
20150008318 | Apparatus and Methods for Ion Mobility Spectrometry - A method of ion mobility spectrometry comprising: (i) introducing a packet of ions into a drift space; (ii) passing the ions through the drift space wherein the ions separate according to their ion mobility; and (iii) reflecting or deflecting the ions that have passed through the drift space back into the drift space wherein the ions can further separate according to their ion mobility. The reflecting or deflecting takes place in a region at lower pressure than the drift space. The drift space may be re-used multiple times to extend the separation path length. The regions of low pressure preferably allow inertial ion motion wherein the mean free path between ion collisions with gas is significantly longer than in the stages of ion mobility separation. The low pressure reflecting or deflecting region enables a time of flight focusing of ions to be provided without ion mobility separation occurring therein. | 01-08-2015 |
20140379279 | Method of Processing Spectrometric Data - A method of characterising a sample from spectrometric data using calculation of spectral distance values is disclosed, for use in the field of mass spectrometry. Molecular formula assignment of peaks in mass spectral data is difficult and time-consuming, and the invention provides a computer implemented method of finding a most likely elemental composition of a measured spectral peak of interest. The method analyses isotopic peaks in a portion of the spectrum, using both their mass positions and intensities, to determine a spectral distance between those peaks and isotopic peaks of a candidate composition, finding peaks that match ( | 12-25-2014 |
20140346343 | Collision Cell - A method of operating a gas-filled collision cell in a mass spectrometer is provided. The collision cell has a longitudinal axis. Ions are caused to enter the collision cell. A trapping field is generated within the collision cell so as to trap the ions within a trapping volume of the collision cell, the trapping volume being defined by the trapping field and extending along the longitudinal axis. Trapped ions are processed in the collision cell and a DC potential gradient is provided, using an electrode arrangement, resulting in a non-zero electric field at all points along the axial length of the trapping volume so as to cause processed ions to exit the collision cell. The electric field along the axial length of the trapping volume has a standard deviation that is no greater than its mean value. | 11-27-2014 |
20140331861 | Mass Spectrometer Vacuum Interface Method and Apparatus - A method of preparing or operating a mass spectrometer vacuum interface comprising a skimmer apparatus having a skimmer aperture and an internal surface of the skimmer apparatus, comprising disposing an adsorbent or getter material on the internal surface. The internal surface has a deposition region where matter from plasma flows may be deposited and the material is disposed on part or all of the deposition region. The disposing step may be performed before a first use and/or intermittently, especially to refresh a previously disposed material. Providing such material serves to trap or collect deposition matter which might anyway be deposited but in such a way that subsequent liberation of that matter is prevented or at least reduced. | 11-13-2014 |
20140326870 | HIGH DUTY CYCLE ION SPECTROMETER - An ion spectrometer is provided, comprising: an ion source, arranged to generate ions continuously with a first range of mass to charge ratios; and an ion trap, arranged to receive ions from the ion source along an axis, and to eject ions with a second range of mass to charge ratios orthogonally to that axis, the second range of mass to charge ratios being narrower than the first range of mass to charge ratios. In some embodiments, ions generated by the ion source continuously flow into the ion trap. Additionally or alternatively, ion optics receive ions ejected from the ion trap and cool the ions without substantial fragmentation. An ion analyser receives ions ejected from the ion trap or ion optics and separates the ions in accordance with at least one characteristic of the ions. | 11-06-2014 |
20140284493 | PREAMPLIFIER FOR CHARGED PARTICLE DETECTION - A preamplifier is provided for correction of overshoot or undershoot effects present in a signal received from a charged particle detection electrode. The preamplifier is ground-isolated from the charged particle detection electrode and comprises: a main amplification stage, configured to receive and amplify the isolated signal; a feed-forward stage, configured to generate a compensation signal from the amplified ground-isolated signal, the compensation signal being generated to mirror the overshoot or undershoot effects; and an output, arranged to provide an output signal that is a combination of the amplified ground-isolated signal and the compensation signal. A charged particle detection arrangement comprising the preamplifier is also provided. | 09-25-2014 |
20140239197 | Electrostatic Trap - An electrostatic trap such as an orbitrap is disclosed, with an electrode structure. An electrostatic trapping field of the form U′(r, φ, z) is generated to trap ions within the trap so that they undergo isochronous oscillations. The trapping field U′(r, φ, z) is the result of a perturbation W to an ideal field U(r, φ, z) which, for example, is hyperlogarithmic in the case of an orbitrap. The perturbation W may be introduced in various ways, such as by distorting the geometry of the trap so that it no longer follows an equipotential of the ideal field U(r, φ, z), or by adding a distortion field (either electric or magnetic). The magnitude of the perturbation is such that at least some of the trapped ions have an absolute phase spread of more than zero but less than 2π radians over an ion detection period T | 08-28-2014 |
20140191122 | Mass Analyser - A mass analyser comprises: an electrical field generator, providing a time-varying electric field for injection of ions to be analysed, excitation of ions to be analysed or both; first and second detection electrodes, each of which receives a respective voltage pickup due to the time-varying electric field and provides a respective detection signal based on a respective image current at the detection electrode; and a differential amplifier, providing an output based on the difference between the detection signal for the first detection electrode and the detection signal for the second detection electrode. It may also be provided that the electrical field generator comprises at least one field generating electrode without a spatially symmetrical counterpart and the capacitance between each field generating electrode and the first detection electrode is substantially the same as the capacitance between that field generating electrode and the second detection electrode. | 07-10-2014 |
20140183352 | Parallel Mass Analysis - A system and method of mass spectrometry is provided. Ions from an ion source are stored in a first ion storage device and in a second ion storage device. Ions are ejected from the first ion storage device to a first mass analysis device during a first ejection time period, for analysis during a first analysis time period. Ions are ejected from the second ion storage device to a second mass analysis device during a second ejection time period. The ion storage devices are connected in series such that an ion transport aperture of the first ion storage device is in communication with an ion transport aperture of the second ion storage device. The first analysis time period and the second ejection time period at least partly overlap. | 07-03-2014 |
20140175274 | Charged Particle Analysers and Methods of Separating Charged Particles - Methods and analysers useful for time of flight mass spectrometry are provided. A method of separating charged particles comprises the steps of:
| 06-26-2014 |
20140166876 | Charged Particle Analysers and Methods of Separating Charged Particles - A method of separating charged particles using an analyser is provided, the method comprising: causing a beam of charged particles to fly through the analyser and undergo within the analyser at least one full oscillation in the direction of an analyser axis (z) of the analyser whilst orbiting about the axis (z) along a main flight path; constraining the arcuate divergence of the beam as it flies through the analyser; and separating the charged particles according to their flight time. An analyser for performing the method is also provided. At least one arcuate focusing lens is preferably used to constrain the divergence, which may comprise a pair of opposed electrodes located either side of the beam. An array of arcuate focusing lenses may be used which are located at substantially the same z coordinate, the arcuate focusing lenses in the array being spaced apart in the arcuate direction and the array extending at least partially around the z axis, thereby constraining the arcuate divergence of the beam a plurality of times as it flies through the analyser. | 06-19-2014 |
20140131567 | Targeted Analysis for Tandem Mass Spectrometry - A tandem mass spectrometer and method are described. Precursor ions are generated in an ion source ( | 05-15-2014 |
20140127823 | Device and Method for Producing CO2, N2 and/or SO2 from a Sample - The invention relates to a device for producing CO | 05-08-2014 |
20140114586 | Method of Improving the Resolution of Compounds Eluted from a Chromatography Device - A method of and apparatus for improving the resolution of compounds eluted from a separation device are disclosed, particularly suited for use in the fields of gas or liquid chromatography. Embodiments of the invention provide that spectroscopic data are measured from an effluent eluted from a chromatography device as a function of elution time; peaks in intensity are identified to form a first set of identified peaks; peaks not due to an eluting compound are discarded from the first set of identified peaks thereby forming a second set of identified peaks from those retained; each peak in the second set of peaks is transformed into a first model peak centered on the elution time of each peak in the second set of peaks; some or all the model peaks created are added together to create a new chromatogram; and all identified peaks in intensity in the second set of peaks having elution times within a given time period of identified peaks in intensity in the new chromatogram are grouped together and assigned to a single eluted compound thereby forming a processed data set. | 04-24-2014 |
20140070091 | Collision Cell - A method of operating a gas-filled collision cell in a mass spectrometer is provided. The collision cell has a longitudinal axis. Ions are caused to enter the collision cell. A trapping field is generated within the collision cell so as to trap the ions within a trapping volume of the collision cell, the trapping volume being defined by the trapping field and extending along the longitudinal axis. Trapped ions are processed in the collision cell and a DC potential gradient is provided, using an electrode arrangement, resulting in a non-zero electric field at all points along the axial length of the trapping volume so as to cause processed ions to exit the collision cell. The electric field along the axial length of the trapping volume has a standard deviation that is no greater than its mean value. | 03-13-2014 |
20140069167 | Device for Providing Gases, in Particular for Isotopic Ratio Analysis - A device is provided for delivering gases to an analyzer, such as an isotopic ratio mass spectrometer. The device includes first and second reactors, preferably arranged in parallel. At least one of the reactors may be selectively activated, or means may be incorporated to circumvent one of the reactors, such that different types of gas conversions may be achieved. | 03-13-2014 |
20140061460 | Method and Apparatus for Mass Analysis - A method of mass analysis and a mass spectrometer are provided wherein a batch of ions is accumulated in a mass analyser; the batch of ions accumulated in the mass analyser is detected using image current detection to provide a detected signal; the number of ions in the batch of ions accumulated in the mass analyser is controlled using an algorithm based on a previous detected signal obtained using image current detection from a previous batch of ions accumulated in the mass analyser; wherein one or more parameters of the algorithm are adjusted based on a measurement of ion current or charge obtained using an independent detector located outside of the mass analyser. | 03-06-2014 |
20120085904 | MASS SPECTROMETER AND METHOD FOR ISOTOPE ANALYSIS - A mass spectrometer for analyzing isotopic signatures, with at least one magnetic analyzer and optionally with an electric analyzer as well, with a first arrangement of ion detectors and/or ion passages and, arranged downstream thereof in the direction of the ion beam, a second arrangement of ion detectors, with at least one deflector in the region of the two arrangements of ion detectors or between these arrangements. Additionally, a multi-collector arrangement, special uses and a method for analyzing isotopes in a sample. The mass spectrometer according to the invention has a control for the at least one deflector such that ion beams of different isotopes can be routed to at least one ion detector in the second arrangement. | 04-12-2012 |
20120006678 | APPARATUS FOR PROVIDING A SUBSTANCE FOR THE ANALYSIS OF ISOTOPE RATIOS - A method and an apparatus for providing a substance for the analysis of isotope ratios, at least some of the substance being contained in a liquid phase in which the liquid phase is subjected to electrolysis and, in the process, the substance or a pre-product for the latter is formed. | 01-12-2012 |
20110086430 | METHOD AND DEVICE FOR ISOTOPIC RATIO ANALYSIS - A process and an apparatus for isotope ratio analysis, the process having the following steps: performing a liquid chromatography process and thus providing an eluate which comprises at least one liquid carrier fluid and at least one analytes, collecting a portion of interest from the eluate, processing the eluate portion to form at least one gaseous conversion products of the analytes, and supplying the gaseous conversion products, especially with gaseous carrier fluid, to an isotope analyzer and determining the isotrope ratios. | 04-14-2011 |
20110024619 | Mass Spectrometer Arrangement with Fragmentation Cell and Ion Selection Device - A method of mass spectrometry having the steps of, in a first cycle: storing sample ions in a first ion storage device; ejecting the stored ions out of the first ion storage device into a separate ion selection device; selecting a subset of the ions in the ion selection device; ejecting the subset of ions selected within the ion selection device to a fragmentation device; directing ions from the fragmentation device back to the first ion storage device without passing them through the said ion selection device; receiving at least some of the ions ejected from the first ion storage device, or their derivatives, back into the first ion storage device; and storing the received ions in the first ion storage device. | 02-03-2011 |
20100224774 | Electrode for influencing ion motion in mass spectrometers - An electrode for influencing ion motion in mass spectrometers, having a dielectric substrate and a conducting layer on portions of the substrate, wherein peripheral borders, edges or convex shapes of the conducting layer adjoin free regions of the substrate. According to the invention, a dielectric layer is provided on transitions from the conducting layer to the adjoining free regions of the substrate such that at least some of the peripheral borders, edges or convex shapes of the conducting layer are covered. | 09-09-2010 |