Velos Pro and Orbitrap Elite

Total Page:16

File Type:pdf, Size:1020Kb

Velos Pro and Orbitrap Elite The Latest Evolution of Ion Trap Technology: Velos Pro and Orbitrap Elite Jae Schwartz Indianapolis Users Meeting September 25, 2011 New Instruments Velos Pro Orbitrap Elite Quadrupole Linear Ion Trap Quadrupole Linear Ion Trap + Orbitrap Hybrid Instrument 2 The Velos Pro - Motivation Feature Application Benefit • UHPLC Cycle Times • More points across a chromatographic peak gives better 1 Faster Scanning quantitative performance • More MSN Scans During a Run, Or Shorter Run • More Information/Unit Time Enhance the Robustness • Improved Robustness to Reduce Instrument Down Time with 2 of Ion Optics High sensitivity S-Lens technology • Single digit RSDs, Competitive Quantitation 3 • Up to 6 orders of linear dynamic range on Ion Traps • First Ion Trap Designed for Quantitation. Improve Dissociation • Increases flexibility for structural elucidation (both proteomics and small molecule applications) 4 No Low mass cut off/TMT • Allows Highly Sensitive TMT Based Protein Quantitation 3 Ion Trap Relationship Between Scan Rate and Peak Width 0.7 0.6 0.5 0.4 0.3 FWHM(amu) 0.2 Scan Rate Range 1 0.1 Scan Rate Range 2 Scan Rate Range 3 0 0 5000 10000 15000 20000 25000 30000 35000 Scan Rate (amu/sec) * At ~1 mtorr 4 New Mass Analysis Scan Rate: “Rapid” Scan Rate 3,500 M/∆M Rapid Ion Ion Ion Mass FWHM=.52 66 KDa/sec Injection Isolation Dissociation Analysis 5,400 M/∆M Normal FWHM=.34 33 KDa/sec n-1 1 7,000 M/∆M Enhanced FWHM=.26 10 KDa/sec 350 INTERSCAN TIME 300 OTHER OVERHEAD MASS ANALYSIS (300-2000) 10,100 M/∆M Zoom 250 ACTIVATION FWHM=.18 ISOLATION 2.2 KDa/sec 200 ION INJECTION PRESCAN 150 36,440 M/∆M 100 FWHM=.05 Ultra Zoom 50 27 Da/sec 0 LTQ XL LTQ VELOS LTQ VELOS w LTQ VELOS PRO P/AGC 5 More Real Scan Speed Improvement: C:\j.horner\...\HCD-N-N-Top20_Short_002 4/21/2011 12:17:21 PM Protein Groups Unique Peptides RT: 0.00 - 130.07 Normal Scan Rate 52.79 NL: 100 3.77E8 Base Peak 9000 8108 80 70.11 MS HCD-N-N- 8000 7477 Top20_Short 60 _002 55.33 7000 40 25.13 35.00 41.32 46.34 64.67 75.91 6000 21.86 28.64 77.28 Relative Abundance 20 4.76 99.52 5.50 82.96 103.13 118.75 5000 0 0 10 20 30 40 50 60 70 80 90 100 110 120 13047061 Scans 4000 Time (min) 3000 1974 HCD-N-N-Top20_Short_002 # 21775 RT: 54.35 AV: 1 NL: 3.95E4 1867 T: ITMS + c NSI d Full ms2 [email protected] [50.00-935.00] 2000 120.01372 1000 30000 460.27264 0 545.33057 660.43414 20000 807.47168 Multiconcensus HCD Multiconcensus HCD Intensity 260.17169 147.04297 Normal Scan Rate Rapid Scan Rate 10000 328.15677 399.20895 201.05994 480.26218 589.37354 692.42554 922.52051 0 100 200 300 400 500 600 700 800 900 C:\j.horner\...\HCDm/z -R-R-Top20_Short_007 4/24/2011 3:56:12 PM Rapid Scan Rate 52.58 69.73 NL: 100 2.60E8 Base Peak 80 MS HCD-R-R- 60 53.90 Top20_Short 40.97 56.75 24.81 64.25 _007 57.19 40 34.58 45.70 75.18 31.53 57.88 Relative Abundance 64.57 82.56 20 4.414.95 13.59 21.57 36.23 48.93 76.54 84.22 94.52 100.54 103.22 115.07118.69 123.10 0 0 10 20 30 40 50 60 70 80 90 100 110 120 130 Up to 10% 52083 Scans Time (min) More Scans 814.37787 250000 961.45288 with Rapid 667.31732 200000 120.07883 150000 157.14017 574.29041 Intensity 100000 504.25012 86.09660 185.08255 50000 267.11484 375.19061 440.22287 559.83539 650.27991712.19629 797.47675 870.48254944.43738 988.43304 1074.53516 1136.89819 0 100 200 300 400 500 600 700 800 900 1000 1100 m/z 6 Velos Pro Speed : Full Ion Tree in 1 second! RT: 6.19 - 6.82 6.44 100 90 80 70 60 50 40 Relative Abundance 30 20 10 0 6.2 6.3 6.4 6.5 6.6 6.7 6.8 Time (min) 8 MSn Spectra in 1 second! 7 SLTQ-Lens Velos Ion Optics- Generation Design: I Ion LTQ Optics Velos • Dual ID Variable Spaced Stacked Lenses: • Larger ID to capture entire expansion from transfer tube • Smaller ID to focus ion beam through conductance limiting aperture • Increasing spacing = increasing field penetration to focus ion beam • Small number of electrodes (18 total in one assembly) • Stainless Steel Electrodes and Supports for Ruggedness and Easy Cleaning • Alternate Phase RF on Lenses (650KHz, 300Vpp max) • Relatively Large Exit Aperture versus Skimmer • 5-10x Transmission Improvement! 8 LTQ Velos - Generation I Ion Optics . “S-LENS” in Velos increased Sensitivity by 10 . Bent Q0 Optics Designed to Catch Neutrals . Can Improve Robustness Further 9 The “Rotated Quadrupole” with neutral beam blocker To prevent material from building up on the rods, the quadrupole has been rotated 450. This opens up a new line of sight for the neutral beam. A beam blocker is now able to capture the neutral beam out side the body of the ion optics! This allows, for the first time, neutrals and ions to be separated in a linear optics design. 10 Velos Pro Ion Optics The majority of material strikes the beam blocker outside of the ion path. 11 Velos Pro Robustness Testing • Using the new rotated Q0, the 100% Velos Pro is 2x as robust as 90% the2x LTQincrease Velos in. 80% robustness averaged 70% ions ions 60% VELOS all 50% PRO 40% 30% 20% Relative Intensity Intensity Relative 10% 0% 0 5 10 15 20 DHB Infused (mg) 12 Ion Traps for Quantitation 1.E+07 1.E+06 1.E+05 Early Ion Traps had a 1.E+04 narrow dynamic range 1.E+03 due to inherent design 1.E+02 limitations Log(SIGNAL) 1.E+01 1.E+00 1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05 1.E+06 1.E+07 Log(Conc) 1.E+07 1.E+06 1.E+05 • Automatic Gain Control 1.E+04 • > 1 0X More Ions 1.E+03 • 1 0 Hz Fast Scanning 1.E+02 • Isolation during loading Log(SIGNAL) High Dynamic Range 1.E+01 • Detection 1.E+00 1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05 1.E+06 1.E+07 Log(Conc) 13 Injection (Isolation) Waveforms With new injection=isolation waveforms, the HPC acts just like a very good single quadrupole! m/z 524 100 80 60 40 20 IsolationEfficiency 0 -8 -7 -6 -5 -4 -3 -2 -1 0 1 2 3 4 5 6 7 8 m/z at Isolation Q Velos symmetric rod stretch Isolation profiles for Velos rf field: E=0 on axis instruments during loading. Even better isolation after loading. 14 Isolation while loading is key 6 3.0x10 5 1.5x10 Select only this ion while 6 2.5x10 5 loading into 1.0x10 the trap! 6 2.0x10 4 5.0x10 6 1.5x10 0.0 710 715 720 725 730 735 740 745 750 Intensity 6 1.0x10 5 5.0x10 0.0 200 400 600 800 1000 Mass 15 Isolation while loading is key Effect of Injection Waveforms: MS/MS of m/z 735 Lactoperoxidase Digest Effect of Injection Waveforms: MS/MS of m/z 735 Off Lactoperoxidase Digest On 105 Waveform OFF Low precursor intensity produces poor quality MS/MS 4 Intensity 10 103 0 50 100 150 200 Waveform ON Scan High precursor intensity Produces high quality MS/MS •Injection waveforms allow selective ion accumulation •Injection waveforms prevent 200 400 600 800 1000 1200 1400 signal variation due to matrix Mass based space charge 16 Faster Scan Rates – Higher Detected Ion Currents 3,500 M/∆M Rapid FWHM=.52 15 usec/amu 5,400 M/∆M Normal FWHM=.34 30 usec/amu 7,000 M/∆M Enhanced FWHM=.26 100 usec/amu 10,100 M/∆M FWHM=.18 Zoom 455 usec/amu 36,440 M/∆M FWHM=.05 Ultra Zoom 3700 usec/amu 17 Continuous Dynode Electron Multiplier (CDEM) Versus Discrete Dynode Electron Multiplier (DDEM) Output electrons ions electrons Glass channel plate Advantages: Advantages: • Smaller . Larger Surface Area • Cost Effective . Each multiplication stage can be optimized . Larger linear Dynamic Range . Longer life times 18 Linear Dynamic Range - 195/196 Intensity Ratio Comparison of High End of Linear Range 12 Old Detection System New Detection System 10 8 Peak RatioPeak ~20 uA ~160 uA 6 4 10 100 Current (µA) 19 New Higher Dynamic Range Detection System • Discreet Dynode Electron Multipliers (ETP-SGE) • Packaged as a Direct Replacement for Previous Continuous channel (Channeltron) Electron Multipliers • Extended dynamic range • Slower aging and longer lifetimes • 24 bit High Dynamic Range Electrometer/Pre Amplifier Circuit • Novel 160 uA electrometer board designed to handle high peak currents found in fast scanning micropackets. (now 24bit) • Packaged to replace current LTQ Velos Electrometer 20 Alprazolam 6 Order Quantification on Velos Pro Pg On RSD% Column 50000 0.01 14.58 40000 30000 0.02 10.76 Area C:\j.horner\...\AlpFull-VelosPro194 4/1/2011 3:55:51 AM 20000 10000 pg on Column Velos Pro 0.04 6.63 RT: 0.00 - 0.80 SM: 7G 10000 Y = 6852.68*X R^2 = 0.9918 W: 1/X 100 0.1 4.25 0 90 0 1 2 3 4 5 6 7 80 pg on Column 0.2 3.21 70 60 0.4 3.70 50 40 Relative Abundance Relative 1 3.59 30 20 10 Alprazolam 2 3.57 0 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 Time (min) 4 3.47 70000000 10 2.48 60000000 20 1.98 RSD 10 fg on Column: 14.58% 50000000 40 4.03 40000000 100 4.33 Area 30000000 200 2.03 400 3.40 20000000 1000 3.85 10000000 Y = 6852.68*X R^2 = 0.9918 W: 1/X 2000 1.66 0 0 2000 4000 6000 8000 10000 4000 1.27 pg on Column 10000 2.16 21 Dynamic Range Summary: 12 Compounds + 1 IS in plasma (5 min run) C:\j.horner\...\ASMS_VelosPro_Run2_088 4/9/2011 12:42:13 PM 200 pg/uL RT:0.00 - 4.40 100 90 2 Scan 80 3 Scan 4 Scan 1 Scan 1 Scan 2 Scan Events Events Events Event Event Events 70 60 50 40 30 20 IS 10 0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 Time (min) Norcodeine 286.30 CID 4 Methampmetamine 150.24 CID 5 Propranolol 260.16 CID >5 Codeine-d3 303.37 CID 5 Methoxymethamphetamine 180.26 CID >5 Alprazolam 309.09 PQD >5 Hydrocodone 300.37 CID >5 Lidocaine 235.34 CID >5 Sulfamethazine 279.09 CID 4 Testosterone 289.43 CID 5 Terfenadine 472.32 CID 6 Methylthioamphetamine 165.22 CID IS 4.2% Bupropion 240.11 CID >5 22 Dissociation Diversity HCD dd Decision Tree ETD CID Complimentary sequence coverage Acronym Long Title Pros/Cons Mechanism CID Collision Induced Dissociation Universal, no tuning required, high Resonance excitation of precursor at low efficiency q; low energy collisions with He Low mass cutoff PQD Pulsed “q” Dissociation Selective, no low mass cutoff, low noise Short resonant excitation of precursor at high q, rapid shift to very low q, high Tuning required, low efficiency energy collisions with He HCD Higher Energy Collision High efficiency, no low mass cutoff Acceleration of ion packet through N2 cell, Induced Dissociation high energy collisions with N2 Tuning required ETD Electron Transfer Dissociation Highly selective, no low mass cutoff, very Transfer of electron from radical low noise destabilizes molecule Doesn’t work on singly charged species 23 Use Existing High Pressure Multipole Collision Cell TRAP-HCD 1.
Recommended publications
  • Mass Spectrometer Detectors
    Mass Spectrometer Detectors www.sge.com Ion Detectors for Virtually all Mass Spectrometry Applications Electron multipliers are used in a wide range of applications to Figure 2. Secondary Electron Emission detect and measure small signals of ions, electrons or photons. One of the main applications for an electron multiplier is for 6 the detection of ions in a mass spectrometer. ACTIVE FILM Multipliers manufactured by ETP ( a division of SGE Group 5 of Companies) are the result of 15 years experience in 4 supplying high performance electron multipliers for use in mass spectrometry applications. The performance of this 3 unique type of ion detector has seen it become widely used in almost all fields of mass spectrometry (including ICP-MS, 2 GC-MS, LC-MS, TOF and SIMS). 1 An electron multiplier is used to detect the presence of ion Secondary Electron Emissions signals emerging from the mass analyser of a mass 0 spectrometer. It is essentially the "eyes" of the instrument (see 0 100 200 300 400 500 Figure 1). The task of the electron multiplier is to detect Incident Electron Energy (eV) every ion of the selected mass passed by the mass filter. How The average number of secondary electrons emitted from the efficiently the electron multiplier carries out this task surface of an ETP electron multiplier plotted against the represents a potentially limiting factor on the overall system energy of the incident primary electron. sensitivity. Consequently the performance of the electron multiplier can have a major influence on the overall (often referred to as a channel electron multiplier or CEM).
    [Show full text]
  • Microchannel Plate Detectors
    Reprinted from Nuclear Instruments and Methods, Vol. 162, 1979, pages 587 to 601 MICROCHANNEL PLATE DETECTORS JOSEPH LADISLAS WIZA 1. Introduction typical. Originally developed as an amplification element for A microchannel plate (MCP) is an array of 104-107 image intensification devices, MCPs have direct sensitivity miniature electron multipliers oriented parallel to one to charged particles and energetic photons which has another (fig. 1); typical channel diameters are in the range extended their usefulness to such diverse fields as X-ray1) 10-100 µm and have length to diameter ratios (α) between and E.U.V.2) astronomy, e-beam fusion studies3) and of 40 and 100. Channel axes are typically normal to, or biased course, nuclear science, where to date most applications at a small angle (~8°) to the MCP input surface. The have capitalized on the superior MCP time resolution channel matrix is usually fabricated from a lead glass, characteristics4-6). treated in such a way as to optimize the secondary emission The MCP is the result of a fortuitous convergence of characteristics of each channel and to render the channel technologies. The continuous dynode electron multiplier walls semiconducting so as to allow charge replenishment was suggested by Farnsworth7) in 1930. Actual from an external voltage source. Thus each channel can be implementation, however, was delayed until the 1960s considered to be a continuous dynode structure which acts when experimental work by Oschepkov et al.8) from the as its own dynode resistor chain. Parallel electrical contact USSR, Goodrich and Wiley9) at the Bendix Research to each channel is provided by the deposition of a metallic Laboratories in the USA, and Adams and Manley10-11) at coating, usually Nichrome or Inconel, on the front and rear the Mullard Research Laboratories in the U.K.
    [Show full text]
  • Characterization of Morphological and Chemical Properties of Scandium Containing
    Characterization of Morphological and Chemical Properties of Scandium Containing Cathode Materials A dissertation presented to the faculty of the College of Arts and Sciences of Ohio University In partial fulfillment of the requirements for the degree Doctor of Philosophy Michael V. Mroz May 2020 © 2020 Michael V. Mroz. All Rights Reserved. 2 This dissertation titled Characterization of Morphological and Chemical Properties of Scandium Containing Cathode Materials by MICHAEL V. MROZ has been approved for the Department of Physics and Astronomy and the College of Arts and Sciences by Martin E. Kordesch Professor of Physics and Astronomy Florenz Plassmann Dean, College of Arts and Sciences 3 ABSTRACT MROZ, MICHAEL V., Ph.D., May 2020, Physics and Astronomy Characterization of Morphological and Chemical Properties of Scandium Containing Cathode Materials Director of Dissertation: Martin E. Kordesch Understanding thermionic cathodes is crucial for the future development of communication technologies operating at the terahertz frequency. Model cathode systems were characterized using multiple experimental techniques. These included Low Energy Electron Microscopy, X-Ray Photoemission Spectroscopy, and Auger Electron Spectroscopy. This was done to determine the mechanisms by which tungsten, barium, scandium, and oxygen may combine in order to achieve high current densities via thermionic emission. Barium and scandium films are found to dewet from the tungsten surfaces studied, and not diffuse out from bulk sources. The dewetted droplets were found to contribute the most to thermal emission. Barium oxide and scandium oxide are also found to react desorb from the emitting surface at lower temperatures then the metals themselves. The function of scandium in scandate cathodes was determined to act as an inhibitor to oxide formation.
    [Show full text]
  • Modern Mass Spectrometry
    Modern Mass Spectrometry MacMillan Group Meeting 2005 Sandra Lee Key References: E. Uggerud, S. Petrie, D. K. Bohme, F. Turecek, D. Schröder, H. Schwarz, D. Plattner, T. Wyttenbach, M. T. Bowers, P. B. Armentrout, S. A. Truger, T. Junker, G. Suizdak, Mark Brönstrup. Topics in Current Chemistry: Modern Mass Spectroscopy, pp. 1-302, 225. Springer-Verlag, Berlin, 2003. Current Topics in Organic Chemistry 2003, 15, 1503-1624 1 The Basics of Mass Spectroscopy ! Purpose Mass spectrometers use the difference in mass-to-charge ratio (m/z) of ionized atoms or molecules to separate them. Therefore, mass spectroscopy allows quantitation of atoms or molecules and provides structural information by the identification of distinctive fragmentation patterns. The general operation of a mass spectrometer is: "1. " create gas-phase ions "2. " separate the ions in space or time based on their mass-to-charge ratio "3. " measure the quantity of ions of each mass-to-charge ratio Ionization sources ! Instrumentation Chemical Ionisation (CI) Atmospheric Pressure CI!(APCI) Electron Impact!(EI) Electrospray Ionization!(ESI) SORTING DETECTION IONIZATION OF IONS OF IONS Fast Atom Bombardment (FAB) Field Desorption/Field Ionisation (FD/FI) Matrix Assisted Laser Desorption gaseous mass ion Ionisation!(MALDI) ion source analyzer transducer Thermospray Ionisation (TI) Analyzers quadrupoles vacuum signal Time-of-Flight (TOF) pump processor magnetic sectors 10-5– 10-8 torr Fourier transform and quadrupole ion traps inlet Detectors mass electron multiplier spectrum Faraday cup Ionization Sources: Classical Methods ! Electron Impact Ionization A beam of electrons passes through a gas-phase sample and collides with neutral analyte molcules (M) to produce a positively charged ion or a fragment ion.
    [Show full text]
  • Joseph Ladislas Wiza, Microchannel Plate Detectors
    Reprinted from Nuclear Instruments and Methods, Vol. 162, 1979, pages 587 to 601 MICROCHANNEL PLATE DETECTORS JOSEPH LADISLAS WIZA 1. Introduction only by the channel dimensions and spacings; 12 mm diameter channels with 15 mm center-to-center spacings are A microchannel plate (MCP) is an array of 104-107 typical. miniature electron multipliers oriented parallel to one Originally developed as an amplification element for another (fig. 1); typical channel diameters are in the range image intensification devices, MCPs have direct sensitivity 10-100 mm and have length to diameter ratios (a) between to charged particles and energetic photons which has 40 and 100. Channel axes are typically normal to, or biased extended their usefulness to such diverse fields as X-ray1) at a small angle (~8°) to the MCP input surface. The and E.U.V.2) astronomy, e-beam fusion studies3) and of channel matrix is usually fabricated from a lead glass, course, nuclear science, where to date most applications treated in such a way as to optimize the secondary emission have capitalized on the superior MCP time resolution characteristics of each channel and to render the channel characteristics4-6). walls semiconducting so as to allow charge replenishment The MCP is the result of a fortuitous convergence of from an external voltage source. Thus each channel can be technologies. The continuous dynode electron multiplier considered to be a continuous dynode structure which acts was suggested by Farnsworth7) in 1930. Actual as its own dynode resistor chain. Parallel electrical contact implementation, however, was delayed until the 1960s to each channel is provided by the deposition of a metallic when experimental work by Oschepkov et al.8) from the coating, usually Nichrome or Inconel, on the front and rear USSR, Goodrich and Wiley9) at the Bendix Research surfaces of the MCP, which then serve as input and output Laboratories in the USA, and Adams and Manley10-11) at electrodes, respectively.
    [Show full text]
  • ELECTRON MULTIPLIERS General Technical Information the Specifications in This Booklet Are Subject to Change
    ELECTRON MULTIPLIERS General Technical Information The specifications in this booklet are subject to change. Please contact ETP for the latest data sheets of any products. PRODUCT DATA 14DM467 500ps MagneTOF® Plus '0SV0DJQH72)£& £ MagneTOF detectorsprovideanexceptionalcombinationof performancecharacteristics.Theyeliminatethecompromises associatedwithotherTOFdetectortechnologies. Thehighperformanceversion,14DM467,typicallyachieves singleionpulsewidthsof<500psFWHM. Specialattentionhasbeengiventominimizingjittersothat pulsesfrommultipleioneventshavenearlythesamewidthas singleionevents. 6SHFLILFDWLRQV ModelNumber 14DM467Rev.H Mechanicalenvelopesize(nominal) 45X52X96mm(notincludingmountingtabs) Inputaperturesize(nominal) 15X33mm <0.55nsMeasuredatdetectoroutputwith3GHz Singleionpulsewidth(FWHM) oscilloscope Ringaftermainpulse(typical) 2%measuredatdetectoroutputwith3GHzoscilloscope Maximumsustainedlinearoutputcurrent 6μAfordispersedorspatiallyconcentratedionbeams Maximumlinearpulseheight 2.5Voltintoa50Ohmload Maximumdarkcounts@2600V <50perminute Recoverytimeafterlargepulse Negligible Maximumoperatingpressure 10Ͳ4Torr Protectfromdustinoriginalpackagingorinan Long/shorttermstoragerequirements appropriatedesiccator MaximumcurrentdrawfromHVpower 0.5mA supplyatthemaximumoperatingVoltage Ambienttemperaturerangefornormal 15to28°C(59to82°F) operation Ambienttemperaturerangeforoptimum 19to23°C(66to73°F) operation Typicalgainwhenmultiplierisnew 1E6@~1950V Operatingvoltagerange* ~Ͳ1800V(initial)toͲ3400Vmaximum(aged). *Note:OperatinganewdetectoratendͲofͲlife(maximum)voltagePD\UHVXOWindamageWRWKHGHWHFWRU
    [Show full text]
  • Photomultiplier Tube Basics Photomultiplier Tube Basics
    Photomultiplier tube basics Photomultiplier tube basics Still setting the standard 8 Figures of merit 18 Single-electron resolution (SER) 18 Construction & operating principle 8 Signal-to-noise ratio 18 The photocathode 9 Timing 18 Quantum efficiency (%) 9 Response pulse width 18 Cathode radiant sensitivity (mA/W) 9 Rise time 18 Spectral response 9 Transit-time and transit-time differences 19 Transit-time spread, time resolution 19 Collection efficiency 11 Very-fast tubes 11 Linearity 19 Fast tubes 11 External factors affecting linearity 19 General-purpose tubes 11 Internal factors affecting linearity 20 Tubes optimized for PHR 12 Linearity measurement 21 Measuring collection efficiency 12 Stability 21 The electron multiplier 12 Long-term drift 21 Secondary emitting dynode coatings 13 Short-term shift (or count rate stability) 22 Voltage dividers 13 Gain 1 Supply and voltage dividers 23 Anode collection space 1 Applying the voltage 23 Anode sensitivity 1 Voltage dividers 2 Specifications and testing 1 Anode resistor 2 Maximum voltage ratings 1 Gain adjustment 2 Anode dark current & dark noise 1 Magnetic fields 2 Ohmic leakage 1 Thermionic emission 1 Magnetic shielding 27 Field emission 1 Environmental considerations 28 Radioactivity 1 Temperature 28 PMT without scintillator 1 Atmosphere 29 PMT with scintillator 1 Mechanical stress 29 Cathode excitation 1 Radiation 29 Dark current values on test tickets 1 Reference 30 Afterpulses 17 www.photonis.com Still setting Construction the standard & operating principle A photomultiplier tube is
    [Show full text]
  • Quadrupole Ion Traps (QIT) • Time-Of-Flight (TOF) Mass Analyzers
    Updated: 17 November 2014 Print version CEE 772: Instrumental Methods in Environmental Analysis Lecture #20 Rosa Yu & Dave Reckhow Mass Spectrometry and Instrumentation CEE 772 #20 1 Content • A brief introduction to mass spectrometry • Mass spectrometry instrumentation – Important MS instrument performance factors – Types of mass spectrometers: • (Triple) Quadrupole Mass Spectrometer • Quadrupole Ion Traps (QIT) • Time-of-flight (TOF) Mass Analyzers Ion source ➡ Mass filtration/separation ➡ Detection CEE 772 #20 2 Content • A brief introduction to mass spectrometry • Mass spectrometry instrumentation – Important MS instrument performance factors – Types of mass spectrometers: • (Triple) Quadrupole Mass Spectrometer • Quadrupole Ion Traps (QIT) • Time-of-flight (TOF) Mass Analyzers Ion source ➡ Mass filtration/separation ➡ Detection CEE 772 #20 3 Mass Spectrometry Introduction Ion Formation Mass Analysis Detection • Ionization: • Electrospray Ionization • Electron Impact/Chemical Ionization • MALDI (matrix assisted laser desorption ionization) • Mass Analysis/Separation: • Use electric and magnetic fields to apply a force on charged particles to control the trajectories of ions • Detection: • Electron multiplier CEE 772 #20 4 The effect of electromagnetic fields on ions • The relationship between force, mass, and the applied fields can be summarized in Newton's second law and the Lorentz force law. 1. Newton's second law: F = ma the force causes an acceleration that is MASS dependent 2. Lorentz force law: F = e(E + vB) the applied force
    [Show full text]
  • Mass Spectrometry
    Mass spectrometry Dr. Kevin R. Tucker What is mass spectrometry? A versatile analytical technique used to determine the Dichloromethane CH2Cl2 12 1 35 composition of chemical C H2 Cl2 = 84 13 1 35 C H2 Cl2 = 85 samples either at the atomic or 12 1 35 37 C H2 Cl Cl = 86 13 1 35 37 molecular level. C H2 Cl Cl = 87 12 1 37 Ionic forms of samples are C H2 Cl2 = 88 separated according to differences in component mass- to-charge (m/z) ratio. Signals from each different isotopic composition Isotope % Natural Abundance m/z Isotopes usually stable 12C 98.93 Keep in mind charge, z, in (+1, +2, 13C 1.07 +3, etc.); not knowing z can result 35Cl 75.77 Textbook value is in mass errors by a factor of 2, 3, a weighted average 37 etc. Cl 24.23 } Cl At. wt. = 35.453 Basic instrumental setup for mass spectrometry Fig. 20-11 Molecular mass spectrometry Chapter 20 Generating ions for molecular mass spectrometry Two major classes Gas phase: Sample vaporized then ionized Desorption: Solid or liquid sample is directly converted into gas phase ions * * * * * Molecular mass spec ion source considerations Gas-phase Thermally stable compounds with bp less than 500oC Limited to masses less than 1000 Da (atomic mass unit; amu) Desorption Does not require volatilization Analytes up to 100,000+ Da Hard vs. soft sources Hard sources leave molecule in excited energy states which relax via bond cleavage. Give “daughter ion” fragments at lower m/z. Soft sources minimize fragmentation. Resulting spectra has fewer peaks.
    [Show full text]
  • Electron Transfer Dissociation and Collision-Induced Dissociation
    ELECTRON TRANSFER DISSOCIATION AND COLLISION-INDUCED DISSOCIATION MASS SPECTROMETRY OF METALLATED OLIGOSACCHARIDES by RANELLE MARIE SCHALLER-DUKE CAROLYN J. CASSADY, COMMITTEE CHAIR JOHN B. VINCENT SHANE C. STREET ŁUKASZ CIEŚLA SHANLIN PAN A DISSERTATION Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Department of Chemistry and Biochemistry in the Graduate School of The University of Alabama TUSCALOOSA, ALABAMA 2019 Copyright Ranelle Marie Schaller-Duke 2019 ALL RIGHTS RESERVED ABSTRACT Investigations of metallated glycans through tandem mass spectrometry (MS/MS) can further the field of glycomics, the sequencing of the human glycome. The field is hindered by the lack of an analytical technique that can determine all the stereo-diverse features of carbohydrates. In this dissertation, electron transfer dissociation (ETD) and collision-induced dissociation (CID) are utilized with metal-adducted oligosaccharides to explore the potential of these techniques to sequence glycans. The resulting mass spectra provide significant insight and information about the structure of oligosaccharides and how to distinguish between these complicated isomeric species. Using univalent, divalent, and trivalent transition metal adducts is valuable to glycan analysis. The ETD process requires multiply charged ions, which do not form via protonation for neutral glycans, and CID of protonated glycans produces uninformative glycosidic bond cleavage. The univalent and trivalent metals investigated did not produce ions sufficient for ETD studies, but CID of the trivalent metal adducts showed significant fragmentation. Dissociation of [M + Met]2+ from the divalent metals formed various fragment ions with ETD producing more cross-ring and internal cleavages, which are necessary for structural analysis.
    [Show full text]
  • LTQ Series Hardware Manual
    LTQ Series Hardware Manual 97055-97072 Revision D September 2015 © 2015 Thermo Fisher Scientific Inc. All rights reserved. Automatic Gain Control, Foundation, Ion Max-S, LTQ XL, Orbitrap Elite, Orbitrap Velos Pro, Velos, Velos Pro, and ZoomScan are trademarks; Unity is a registered service mark; and Accela, Ion Max, LTQ, LXQ, Orbitrap, Thermo Scientific, and Xcalibur are registered trademarks of Thermo Fisher Scientific Inc. in the United States. The following are registered trademarks in the United States and other countries: Microsoft and Windows are registered trademarks of Microsoft Corporation. Vespel is a registered trademark of E.I. du Pont de Nemours &Co. The following are registered trademarks in the United States and possibly other countries: Agilent is a registered trademark of Agilent Technologies, Inc. Convectron is a registered trademark of Helix Technology Corporation. Liquinox is a registered trademark of Alconox, Inc. MICRO-MESH is a registered trademark of Micro-Surface Finishing Products, Inc. Upchurch Scientific is a registered trademark of IDEX Health & Science LLC. Viton is a registered trademark of DuPont Performance Elastomers LLC. Waters is a registered trademark of Waters Corporation. All other trademarks are the property of Thermo Fisher Scientific Inc. and its subsidiaries. Thermo Fisher Scientific Inc. provides this document to its customers with a product purchase to use in the product operation. This document is copyright protected and any reproduction of the whole or any part of this document is strictly prohibited, except with the written authorization of Thermo Fisher Scientific Inc. The contents of this document are subject to change without notice. All technical information in this document is for reference purposes only.
    [Show full text]
  • Mass Spectrometry 3
    PLATINblue MSQ Plus Hardware Guide V6950A UHPLC/HPLC Mass spectrometry 3 Content Preface . 8 Safety . 8 Fuses . 8 Lab regulations . 8 LC Solvents and Mobile Phase Additives . 8 LC Solvents . 8 Protective measures . 9 Safety precautions . 9 Solvent and Gas Purity Requirements . 11 Contacting Us . 11 To contact Technical Support or Customer Service for ordering information . 11 To suggest changes to documentation or to Help . 11 Introduction . 12 Overview . 12 Ion Polarity Modes . 13 Ionization Techniques . 14 Electrospray Ionization (ESI) . 14 Ion Desolvation Mechanism . 14 Spectral Characteristics . 15 Atmospheric Pressure Chemical Ionization (APCI) . 16 Ion Generation Mechanism . 16 Spectral Characteristics . 18 Scan Types . 18 Full Scan . 18 Selected Ion Monitoring (SIM) . 18 Data Types . 19 Profile Data Type . 19 Centroid Data Type . 20 MCA Data Type . 21 Functional Description. 22 Liquid Chromatograph . 23 To open the Instrument Configuration application . 23 Reference Inlet System . 25 Mass Detector . 27 Front Panel Status Indicator . 28 Rear Panel Controls and Connections . 29 Connection Between LC and Mass Detector . 31 API Sources . 31 V6950A 4 Electrospray Ionization (ESI) . 31 Atmospheric Pressure Chemical Ionization (APCI) . 33 RF/dc Prefilter . 34 Mass Analyzer . 35 RF and DC Fields Applied to the Quadrupoles . 35 Mass Analysis . 36 Ion Detection System . 37 Vacuum System . 39 Vacuum Manifold . 40 Turbomolecular Pump . 40 Forepump . 41 Pirani Gauge . 41 Vent Valve . 41 Inlet Gas Hardware . 42 Cone Wash System . 45 Data System . 46 Computer Hardware . 46 Xcalibur Software . 47 MSQ Plus Mass Detector Server . 49 Tune Window . 50 Title Bar . 51 Menu Bar . 51 Toolbar . 51 Comms Indicator . 51 Scan Events Table .
    [Show full text]