CA2509525C - Icp-oes and icp-ms induction current - Google Patents
Icp-oes and icp-ms induction current Download PDFInfo
- Publication number
- CA2509525C CA2509525C CA2509525A CA2509525A CA2509525C CA 2509525 C CA2509525 C CA 2509525C CA 2509525 A CA2509525 A CA 2509525A CA 2509525 A CA2509525 A CA 2509525A CA 2509525 C CA2509525 C CA 2509525C
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- CA
- Canada
- Prior art keywords
- plasma
- set forth
- generating
- magnetic field
- current
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 230000006698 induction Effects 0.000 title description 3
- 238000000034 method Methods 0.000 claims abstract description 16
- 230000003595 spectral effect Effects 0.000 claims abstract description 6
- 239000000463 material Substances 0.000 claims description 12
- 239000012159 carrier gas Substances 0.000 claims description 9
- 239000007789 gas Substances 0.000 claims description 3
- 238000002354 inductively-coupled plasma atomic emission spectroscopy Methods 0.000 description 9
- 238000010586 diagram Methods 0.000 description 6
- 238000001095 inductively coupled plasma mass spectrometry Methods 0.000 description 6
- 238000009616 inductively coupled plasma Methods 0.000 description 4
- 230000005284 excitation Effects 0.000 description 3
- 238000004458 analytical method Methods 0.000 description 2
- 239000007921 spray Substances 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000000295 emission spectrum Methods 0.000 description 1
- 150000002500 ions Chemical class 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 239000006199 nebulizer Substances 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 238000004611 spectroscopical analysis Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J49/00—Particle spectrometers or separator tubes
- H01J49/02—Details
- H01J49/10—Ion sources; Ion guns
- H01J49/105—Ion sources; Ion guns using high-frequency excitation, e.g. microwave excitation, Inductively Coupled Plasma [ICP]
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/71—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited
- G01N21/73—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited using plasma burners or torches
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- H05H1/00—Generating plasma; Handling plasma
- H05H1/24—Generating plasma
- H05H1/26—Plasma torches
- H05H1/30—Plasma torches using applied electromagnetic fields, e.g. high frequency or microwave energy
Abstract
In a method of spectroscopically analyzing a sample (104), a plasma (116) is generated. A magnetic field is generated by a magnetic dipole wherein the plasma is confined within the magnetic field. Sample atoms are introduced into the plasma wherein energized atoms of the sample are confined. The spectral composition or mass-to-charge ratio of the energized sample atoms is analyzed.
In a spectroscopic system a magnetic dipole has an associated magnetic field.
A plasma is confined within the magnetic field and a sample of energized atoms introduced into the plasma. A spectrometer (120) analyzes the energized atoms for the mass-to-charge ratio or for their spectral composition.
In a spectroscopic system a magnetic dipole has an associated magnetic field.
A plasma is confined within the magnetic field and a sample of energized atoms introduced into the plasma. A spectrometer (120) analyzes the energized atoms for the mass-to-charge ratio or for their spectral composition.
Description
=
ICP-OES AND ICP-MS INDUCTION CURRENT
Field Of The Invention [0002] This invention relates to a method and apparatus for spectroscopically analyzing a material sample in a plasma.
Background Of The Invention [0003] Conventional Inductively Coupled Plasma-Optical Emission Spectroscopy ICP-OES and Inductively Coupled Plasma-Atomic Emission Spectroscopy ICP-MS systems typically utilize a solenoid receptive of an RF
electrical current for confining a plasma and material sample in an associated magnetic field for analysis. However, such a device generates an uneven magnetic field over the length of the interior of the solenoid due to the helical configuration of the solenoid. This results in an uneven temperature distribution within the plasma affecting sample excitation and the trajectory of ions in the plasma. In addition, the solenoid is a single element, which lacks flexibility in controlling the associated magnetic field and the plasma/sample excitation.
Summary Of The Invention [0004] In a method of spectroscopically analyzing a sample, a plasma is generated. A magnetic field is generated by a magnetic dipole wherein the plasma is confined within the magnetic field. Atoms of a material sample are introduced into the plasma wherein energized atoms of the sample are at least temporarily confined. The spectral or mass content of the energized sample atoms are analyzed.
ICP-OES AND ICP-MS INDUCTION CURRENT
Field Of The Invention [0002] This invention relates to a method and apparatus for spectroscopically analyzing a material sample in a plasma.
Background Of The Invention [0003] Conventional Inductively Coupled Plasma-Optical Emission Spectroscopy ICP-OES and Inductively Coupled Plasma-Atomic Emission Spectroscopy ICP-MS systems typically utilize a solenoid receptive of an RF
electrical current for confining a plasma and material sample in an associated magnetic field for analysis. However, such a device generates an uneven magnetic field over the length of the interior of the solenoid due to the helical configuration of the solenoid. This results in an uneven temperature distribution within the plasma affecting sample excitation and the trajectory of ions in the plasma. In addition, the solenoid is a single element, which lacks flexibility in controlling the associated magnetic field and the plasma/sample excitation.
Summary Of The Invention [0004] In a method of spectroscopically analyzing a sample, a plasma is generated. A magnetic field is generated by a magnetic dipole wherein the plasma is confined within the magnetic field. Atoms of a material sample are introduced into the plasma wherein energized atoms of the sample are at least temporarily confined. The spectral or mass content of the energized sample atoms are analyzed.
[0005] In a spectroscopic system a magnetic dipole has an associated magnetic field. A plasma is confined within the magnetic field and a material sample of atoms is introduced into the plasma. A spectrometer analyzes the excited atoms for their mass-to-charge ratio or for their emission spectra.
Brief Description Of The Drawings [0006] FIG. 1 is schematic diagram of an Inductively Coupled Plasma-Optical Emission Spectroscopy (ICP-OES) system.
Brief Description Of The Drawings [0006] FIG. 1 is schematic diagram of an Inductively Coupled Plasma-Optical Emission Spectroscopy (ICP-OES) system.
[0007] FIG. 2 is schematic diagram of an Inductively Coupled Plasma-Mass Spectroscopy (ICP-MS) system.
[0008] FIG. 3 is a diagram of an ICP torch and a plasma.
[0009] FIG. 4 is a side view of two electrodes of the invention and an ICP torch and a plasma.
[0010] FIG. 5 is a front view of an electrode for controlling a plasma, the electrode including an aperture.
[0011] FIG. 6 is a front view of an electrode for controlling a plasma, the electrode including an aperture.
[0012] FIG. 7 is a side view of the electrodes of Fig. 6.
[0013] FIG. 8 is a three dimensional view of a single piece electrode of the invention.
[0014] FIG. 9 is a front view of the single piece electrode of Fig. 8.
[0015] FIG. 10 is a side view of the single piece electrode of Fig. 8.
[0016] FIG. 11 is a top view of the single piece electrode of Fig. 8.
[0017] FIG. 12 is a three dimensional view of a magnetic field generated from a loop current.
[0018] FIG. 13 is a diagram of an ICP torch showing the helical nature of a solenoid.
[0019] FIG. 14 is a diagram of a plurality of loop currents driven by a single RF power source during alternating half cycles of a sinusoidally alternating current..
Detailed Description Of The Drawings [0020] FIG. I shows a schematic diagram of an Inductively Coupled Plasma-Optical Emission Spectroscopy (ICP-OES) system at 100. The ICP-OES 100 generally comprises a system for directing a carrier gas 102 to a torch 114 whereat the carrier gas 102 is ionized to form a hot plasma 116 (5,000 -10,000K). The plasma 116 comprises a preheating zone 190, an induction zone 192, an initial radiation zone 194, an analytic zone 196 and a plasma tail 198. An atomized sample 104 is also directed to the plasma 116 through a pump 106, nebulizer 108 and spray chamber 162. A radio frequency (RF) power source 110 provides RF electrical power to the plasma 116 by way of a load coil 112.
Detailed Description Of The Drawings [0020] FIG. I shows a schematic diagram of an Inductively Coupled Plasma-Optical Emission Spectroscopy (ICP-OES) system at 100. The ICP-OES 100 generally comprises a system for directing a carrier gas 102 to a torch 114 whereat the carrier gas 102 is ionized to form a hot plasma 116 (5,000 -10,000K). The plasma 116 comprises a preheating zone 190, an induction zone 192, an initial radiation zone 194, an analytic zone 196 and a plasma tail 198. An atomized sample 104 is also directed to the plasma 116 through a pump 106, nebulizer 108 and spray chamber 162. A radio frequency (RF) power source 110 provides RF electrical power to the plasma 116 by way of a load coil 112.
[0021] While in the plasma 116 excited sample atoms 104 give off light 134 as they decay to a lower state. The light 134 is collected by collection optics 118 and directed to a spectrometer 120 where it is spectrally resolved. A detector 122 detects the spectrally resolved light 134 and provides a signal 138, 140 to a microprocessor 122 and computer network 124 for analysis. In FIG. 1 it is seen that the viewing of the plasma 116 is from a direction at a right angle to the plasma 116. However, it will be understood from FIG. 1 that the viewing of the plasma 116 may also be performed from a direction along the axis 126. It will also be understood that the Inductively Coupled Plasma Spectroscopy performed herein may also be performed with a mass spectrometer (MS) 180 such as a quadrupole mass analyzer in an Inductively Coupled Plasma-Mass Spectroscopy (ICP-MS) system at 100 as seen in FIG. 2. The RF power source 110 operates generally in the range of 10 to 100 MHz, particularly 20 - 50 MHz, e.g., 27 -40 MHz.
[0022] FIG. 3 shows a more detailed rendition of the plasma 116 of FIGS. 1 and 2. The torch 114 includes three concentric tubes 114, 150, 148.
The innermost tube 148, provides atomized flow 146 of the sample into the plasma 116. The middle tube 150, provides auxiliary gas flow 144 to the plasma 116. The outermost tube 114, provides carrier gas flow 128 for sustaining the plasma. The carrier gas flow 128 is directed to the plasma 116 in an laminar flow about the middle tube 150. The auxiliary gas flow 144 is directed to the plasma 116 within the middle tube 150 and the atomized sample flow 146 is directed to the plasma 116 from the spray chamber 162 along the innermost tube 148. The RF current 130, 132 in the load coil 112 forms a magnetic field within the load coil 112 so as to confine the plasma therein.
The innermost tube 148, provides atomized flow 146 of the sample into the plasma 116. The middle tube 150, provides auxiliary gas flow 144 to the plasma 116. The outermost tube 114, provides carrier gas flow 128 for sustaining the plasma. The carrier gas flow 128 is directed to the plasma 116 in an laminar flow about the middle tube 150. The auxiliary gas flow 144 is directed to the plasma 116 within the middle tube 150 and the atomized sample flow 146 is directed to the plasma 116 from the spray chamber 162 along the innermost tube 148. The RF current 130, 132 in the load coil 112 forms a magnetic field within the load coil 112 so as to confine the plasma therein.
[0023] FIGS. 4 - 11 show various configurations of an electrode 152, 156, 158. In FIG. 4 the electrode 152 comprises two parallel plates 152x, 152b positioned at a distance 'L' from one another. The parallel plates-152a, 152b each include an aperture 154 through which the torch 114 is positioned such that the torch 114, the innermost tube 148, the middle tube 150 and the aperture 154 are aligned along an axis 126. The parallel plates 152a, 152b have a thickness of 't.' The aperture 154 of the electrode 152 also includes a slot 164, of width 'w' such that the aperture 154 is in communication with its surroundings.
[0024] As seen in FIGS. 4 and 5, the electrode 152 is generally comprised of a square or rectangular planar shape, though it may be a wire as seen in FIG. 12. In FIG. 5 it will be appreciated that the RF current supplied to the planar electrode comprises a planar current loop 172a generating a toroidal magnetic field 182 through the aperture 154 (FIG. 12).
In FIGS. 6 and 7 the electrode 156 is of a rounded nature having an outside diameter of D, and inside aperture diameter of D2. The electrodes 152, 156 of FIGS. 4 - 7 are distinct elements which are supplied independently with RF
electrical current 172 of opposite polarity. One part 176 of the electrode 152 is supplied with the RF power while a second part 178 of the electrode 152 is tied to a ground 174. Thus, during arc ignition of the plasma 116, if the ignition arc makes contact with electrode 152, any unwanted electric currents set up in the electrode 152 will be directed to the ground point 174 and not through to the RF power supply 110. The RF power and frequency supplied to each electrode 152 can be independently controlled and varied for optimum performance. For instance, each electrode 152 can be driven at a different frequency in order to optimize the plasma emission and excitation. In addition, one electrode can be operated in a continuous power mode while the other electrode can be modulated (e.g.; pulsed or gated). Furthermore, the distance, 'L', between the electrodes 152 can be adjusted since the electrodes 152 are not connected to one another; thus adjusting the power distribution within the plasma 116. Yet further, the diameter, D2, of the aperture 154 can be independently adjusted in order to adjust the coupling characteristics between the RF power supply 110 and the plasma 116. In FIGS. 8 - 11 the electrode 158 is shown as a single element having-two electrodes 166, 168 connected to a common electrical ground 170.
In FIGS. 6 and 7 the electrode 156 is of a rounded nature having an outside diameter of D, and inside aperture diameter of D2. The electrodes 152, 156 of FIGS. 4 - 7 are distinct elements which are supplied independently with RF
electrical current 172 of opposite polarity. One part 176 of the electrode 152 is supplied with the RF power while a second part 178 of the electrode 152 is tied to a ground 174. Thus, during arc ignition of the plasma 116, if the ignition arc makes contact with electrode 152, any unwanted electric currents set up in the electrode 152 will be directed to the ground point 174 and not through to the RF power supply 110. The RF power and frequency supplied to each electrode 152 can be independently controlled and varied for optimum performance. For instance, each electrode 152 can be driven at a different frequency in order to optimize the plasma emission and excitation. In addition, one electrode can be operated in a continuous power mode while the other electrode can be modulated (e.g.; pulsed or gated). Furthermore, the distance, 'L', between the electrodes 152 can be adjusted since the electrodes 152 are not connected to one another; thus adjusting the power distribution within the plasma 116. Yet further, the diameter, D2, of the aperture 154 can be independently adjusted in order to adjust the coupling characteristics between the RF power supply 110 and the plasma 116. In FIGS. 8 - 11 the electrode 158 is shown as a single element having-two electrodes 166, 168 connected to a common electrical ground 170.
[0025] In FIG. 14 a plurality of loop currents 184a, 184b is shown generated from a single RF electric current source 110. The loop currents 184a, 184b are oriented with respect to one another in such a manner that the alternating electric current in a first loop current 184a flows in a direction opposite to that of the alternating electric current in a second loop current 184b during alternating half cycles of a sinusoidally alternating current.
This allows for the plurality of loop currents 184a, 184b to be driven from a single power source 110 so as to generate magnetic fields 182a, 182b having the same spatial orientation.
This allows for the plurality of loop currents 184a, 184b to be driven from a single power source 110 so as to generate magnetic fields 182a, 182b having the same spatial orientation.
[0026] While the invention has been described above in detail with reference to specific embodiments, various changes and modifications which fall within the spirit of the invention and the scope of the claims will become apparent to those skilled in the art. Therefore, the invention is intended to be limited only by the appended claims and their equivalents.
[0027] Thus, based upon the foregoing description, a method and apparatus for spectroscopically analyzing a sample is disclosed. The method comprises generating a plasma; generating a magnetic field by a magnetic dipole wherein the plasma is confined within the magnetic field; introducing sample atoms into the plasma wherein excited sample atoms are confined;
and analyzing the spectral or mass content of the excited sample atoms.
and analyzing the spectral or mass content of the excited sample atoms.
[0028] Furthermore, a spectroscopic system comprises a magnetic dipole having an associated magnetic field; a plasma confined within the magnetic field; a sample of excited atoms introduced within the plasma; and a spectrometer for analyzing the spectral or mass content of the excited sample atoms.
Claims (17)
1. A method of spectroscopically analyzing a material sample, the method comprising:
generating a plasma;
generating a sinusoidally alternating electric loop current so as to generate a magnetic field, wherein the plasma is confined within the magnetic field;
introducing atoms of the material sample into the plasma wherein excited sample atoms are confined; and analyzing characteristic features of the excited sample atoms, wherein the step of generating a loop current comprises generating a planar loop current.
generating a plasma;
generating a sinusoidally alternating electric loop current so as to generate a magnetic field, wherein the plasma is confined within the magnetic field;
introducing atoms of the material sample into the plasma wherein excited sample atoms are confined; and analyzing characteristic features of the excited sample atoms, wherein the step of generating a loop current comprises generating a planar loop current.
2. The method as set forth in Claim 1 wherein generating a sinusoidally alternating electric current comprises generating a radio frequency electric current.
3. The method as set forth in Claim 1 wherein analyzing characteristic features of the excited sample atoms comprises analyzing the spectral composition or mass-to-charge ratio of the excited sample atoms.
4. The method as set forth in Claim 1 further comprising electrically grounding the loop current.
5. The method as set forth in Claim 1 wherein the loop defines an aperture.
6. The method as set forth in Claim 1 wherein generating a loop current comprises generating a plurality of loop currents.
7. The method as set forth in Claim 6 wherein generating a plurality of loop currents comprises generating a plurality of parallel or antiparallel loop currents separated by a prescribed distance.
8. The method as set forth in Claim 7 wherein the alternating electric current in a first loop current flows in a direction opposite to that of the alternating electric current in a second loop current during alternating half cycles of the sinusoidally alternating current.
9. The method as set forth in Claim 5 further comprising adjusting an area of the aperture.
10. The method as set forth in Claim 7 further comprising adjusting the prescribed distance.
11. A spectroscopic system comprising:
an electric current source for generating a sinusoidally alternating electric loop current, said loop current having an associated magnetic field;
a plasma gas generator for generating a plasma at least in part by a carrier gas flow introduced within the magnetic field via a carrier gas conduit, said plasma confined within the magnetic field;
a material sample conduit for introducing a material sample into the plasma, the atoms of said material sample being excited within the plasma;
and a spectrometer for analyzing characteristic features of the excited atoms;
wherein the sinusoidally alternating electric loop current comprises a planar loop current.
an electric current source for generating a sinusoidally alternating electric loop current, said loop current having an associated magnetic field;
a plasma gas generator for generating a plasma at least in part by a carrier gas flow introduced within the magnetic field via a carrier gas conduit, said plasma confined within the magnetic field;
a material sample conduit for introducing a material sample into the plasma, the atoms of said material sample being excited within the plasma;
and a spectrometer for analyzing characteristic features of the excited atoms;
wherein the sinusoidally alternating electric loop current comprises a planar loop current.
12. The spectroscopic system as set forth in Claim 11 wherein the sinusoidally alternating electric current is a radio frequency current.
13. The spectroscopic system as set forth in Claim 11 wherein the loop current defines an aperture.
14. The spectroscopic system as set forth in Claim 11 wherein the loop current comprises a plate.
15. The spectroscopic system as set forth in Claim 11 wherein the loop current comprises a plurality of plates.
16. The spectroscopic system as set forth in Claim 15 wherein the plurality of plates are parallel.
17. A spectroscopic system comprising:
an electric current source for generating a sinusoidally alternating planar electric loop current, the planar loop current having an associated magnetic field;
a carrier gas conduit for introducing a carrier gas within the magnetic field, said carrier gas for sustaining a plasma generated within a magnetic field;
a material sample conduit for introducing the atomized material sample into the plasma, and;
a spectrometer positioned in the vicinity of the plasma for analyzing characteristic features of excited atoms of the material sample.
an electric current source for generating a sinusoidally alternating planar electric loop current, the planar loop current having an associated magnetic field;
a carrier gas conduit for introducing a carrier gas within the magnetic field, said carrier gas for sustaining a plasma generated within a magnetic field;
a material sample conduit for introducing the atomized material sample into the plasma, and;
a spectrometer positioned in the vicinity of the plasma for analyzing characteristic features of excited atoms of the material sample.
Applications Claiming Priority (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US43296302P | 2002-12-12 | 2002-12-12 | |
| US60/432,963 | 2002-12-12 | ||
| US10/730,779 | 2003-12-09 | ||
| US10/730,779 US7106438B2 (en) | 2002-12-12 | 2003-12-09 | ICP-OES and ICP-MS induction current |
| PCT/US2003/039440 WO2004055493A2 (en) | 2002-12-12 | 2003-12-11 | Icp-oes and icp-ms induction current |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CA2509525A1 CA2509525A1 (en) | 2004-07-01 |
| CA2509525C true CA2509525C (en) | 2011-03-22 |
Family
ID=32912132
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA2509525A Expired - Lifetime CA2509525C (en) | 2002-12-12 | 2003-12-11 | Icp-oes and icp-ms induction current |
Country Status (7)
| Country | Link |
|---|---|
| US (1) | US7106438B2 (en) |
| EP (1) | EP1570254B1 (en) |
| JP (1) | JP4290161B2 (en) |
| CN (1) | CN100529741C (en) |
| AU (1) | AU2003293514B2 (en) |
| CA (1) | CA2509525C (en) |
| WO (1) | WO2004055493A2 (en) |
Families Citing this family (18)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7511246B2 (en) * | 2002-12-12 | 2009-03-31 | Perkinelmer Las Inc. | Induction device for generating a plasma |
| DE102004022200B4 (en) * | 2004-05-05 | 2006-07-20 | Actinium Pharmaceuticals, Inc. | Radium target and process for its preparation |
| AU2006223254B2 (en) * | 2005-03-11 | 2012-04-26 | Perkinelmer U.S. Llc | Plasmas and methods of using them |
| US7742167B2 (en) * | 2005-06-17 | 2010-06-22 | Perkinelmer Health Sciences, Inc. | Optical emission device with boost device |
| US8622735B2 (en) * | 2005-06-17 | 2014-01-07 | Perkinelmer Health Sciences, Inc. | Boost devices and methods of using them |
| US20070046934A1 (en) * | 2005-08-26 | 2007-03-01 | New Wave Research, Inc. | Multi-function laser induced breakdown spectroscopy and laser ablation material analysis system and method |
| DE102006008023B4 (en) | 2006-02-21 | 2008-05-29 | Actinium Pharmaceuticals, Inc. | Method of cleaning 225Ac from irradiated 226Ra targets |
| EP2796575B8 (en) * | 2006-09-08 | 2020-04-01 | Actinium Pharmaceuticals, Inc. | Method for the purification of radium from different sources |
| US20110108058A1 (en) * | 2009-11-11 | 2011-05-12 | Axcelis Technologies, Inc. | Method and apparatus for cleaning residue from an ion source component |
| US8786394B2 (en) | 2010-05-05 | 2014-07-22 | Perkinelmer Health Sciences, Inc. | Oxidation resistant induction devices |
| CA2796815C (en) | 2010-05-05 | 2019-06-25 | Perkinelmer Health Sciences, Inc. | Inductive devices and low flow plasmas using them |
| US8563924B2 (en) * | 2011-06-28 | 2013-10-22 | Agilent Technologies, Inc. | Windowless ionization device |
| WO2014011919A2 (en) | 2012-07-13 | 2014-01-16 | Perkinelmer Health Sciences, Inc. | Torches and methods of using them |
| AU2015211303B2 (en) * | 2014-01-28 | 2019-07-25 | Perkinelmer U.S. Llc | Induction devices and methods of using them |
| US9165751B1 (en) | 2014-06-06 | 2015-10-20 | Agilent Technologies, Inc. | Sample atomization with reduced clogging for analytical instruments |
| US9673032B1 (en) | 2016-03-31 | 2017-06-06 | Agilent Technologies Inc. | Sample sprayer with adjustable conduit and related methods |
| US10300551B2 (en) * | 2016-11-14 | 2019-05-28 | Matthew Fagan | Metal analyzing plasma CNC cutting machine and associated methods |
| US10195683B2 (en) * | 2016-11-14 | 2019-02-05 | Matthew Fagan | Metal analyzing plasma CNC cutting machine and associated methods |
Family Cites Families (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4540884A (en) * | 1982-12-29 | 1985-09-10 | Finnigan Corporation | Method of mass analyzing a sample by use of a quadrupole ion trap |
| US4629940A (en) | 1984-03-02 | 1986-12-16 | The Perkin-Elmer Corporation | Plasma emission source |
| US4818916A (en) | 1987-03-06 | 1989-04-04 | The Perkin-Elmer Corporation | Power system for inductively coupled plasma torch |
| US4766287A (en) | 1987-03-06 | 1988-08-23 | The Perkin-Elmer Corporation | Inductively coupled plasma torch with adjustable sample injector |
| GB9203463D0 (en) | 1992-02-19 | 1992-04-08 | Applied Res Lab | Method and apparatus for analytical sample preparation |
| WO1994006263A1 (en) * | 1992-09-01 | 1994-03-17 | The University Of North Carolina At Chapel Hill | High pressure magnetically assisted inductively coupled plasma |
| US5526110A (en) | 1994-07-08 | 1996-06-11 | Iowa State University Research Foundation, Inc. | In situ calibration of inductively coupled plasma-atomic emission and mass spectroscopy |
| EP0792091B1 (en) | 1995-12-27 | 2002-03-13 | Nippon Telegraph And Telephone Corporation | Elemental analysis method |
| JP2929275B2 (en) * | 1996-10-16 | 1999-08-03 | 株式会社アドテック | Inductively coupled planar plasma generator with permeable core |
| US6329757B1 (en) | 1996-12-31 | 2001-12-11 | The Perkin-Elmer Corporation | High frequency transistor oscillator system |
-
2003
- 2003-12-09 US US10/730,779 patent/US7106438B2/en active Active
- 2003-12-11 JP JP2005508319A patent/JP4290161B2/en not_active Expired - Lifetime
- 2003-12-11 CA CA2509525A patent/CA2509525C/en not_active Expired - Lifetime
- 2003-12-11 CN CNB2003801095259A patent/CN100529741C/en not_active Expired - Lifetime
- 2003-12-11 EP EP03790465.3A patent/EP1570254B1/en not_active Expired - Lifetime
- 2003-12-11 WO PCT/US2003/039440 patent/WO2004055493A2/en active IP Right Grant
- 2003-12-11 AU AU2003293514A patent/AU2003293514B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| US20040169855A1 (en) | 2004-09-02 |
| US7106438B2 (en) | 2006-09-12 |
| WO2004055493A3 (en) | 2004-12-09 |
| EP1570254A2 (en) | 2005-09-07 |
| CN1745295A (en) | 2006-03-08 |
| CN100529741C (en) | 2009-08-19 |
| EP1570254A4 (en) | 2007-01-03 |
| AU2003293514B2 (en) | 2007-07-19 |
| JP4290161B2 (en) | 2009-07-01 |
| AU2003293514A1 (en) | 2004-07-09 |
| JP2006516325A (en) | 2006-06-29 |
| EP1570254B1 (en) | 2020-11-18 |
| AU2003293514B8 (en) | 2004-07-09 |
| CA2509525A1 (en) | 2004-07-01 |
| WO2004055493A2 (en) | 2004-07-01 |
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| Date | Code | Title | Description |
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| EEER | Examination request | ||
| MKEX | Expiry |
Effective date: 20231211 |