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GB2127212A - Apparatus for producing sample ions - Google Patents

Apparatus for producing sample ions Download PDF

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Publication number
GB2127212A
GB2127212A GB08320542A GB8320542A GB2127212A GB 2127212 A GB2127212 A GB 2127212A GB 08320542 A GB08320542 A GB 08320542A GB 8320542 A GB8320542 A GB 8320542A GB 2127212 A GB2127212 A GB 2127212A
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United Kingdom
Prior art keywords
sample
needle
emitter
electrode
pointed end
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.)
Granted
Application number
GB08320542A
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GB2127212B (en
GB8320542D0 (en
Inventor
Hirofumi Kuwabara
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Individual
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Individual
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Filing date
Publication date
Priority claimed from JP57143255A external-priority patent/JPS5936385B2/en
Priority claimed from JP57143254A external-priority patent/JPS5935347A/en
Application filed by Individual filed Critical Individual
Publication of GB8320542D0 publication Critical patent/GB8320542D0/en
Publication of GB2127212A publication Critical patent/GB2127212A/en
Application granted granted Critical
Publication of GB2127212B publication Critical patent/GB2127212B/en
Expired legal-status Critical Current

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J49/00Particle spectrometers or separator tubes
    • H01J49/02Details
    • H01J49/10Ion sources; Ion guns
    • H01J49/16Ion sources; Ion guns using surface ionisation, e.g. field-, thermionic- or photo-emission

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Other Investigation Or Analysis Of Materials By Electrical Means (AREA)

Abstract

Apparatus for producing sample ions comprising means of producing metastable species by corona discharge 17 in a carrier gas, a needle-shaped emitter 22 whose pointed end is inserted into the stream of carrier gas which transports said metastable species, means 23 for applying a high potential to said needle emitter, wherein sample S is arranged adjacent to or deposited on the pointed end of said emitter. May supply sample ions to a mass spectrometer 32. <IMAGE>

Description

SPECIFICATION Apparatus for producing sample ions The present invention relates to apparatus for producing sample ions, particularly for use with a mass spectrometer.
Prior to this invention, the present inventor had proposed a new apparatus and method for producing sample ions, both of which are fully disclosed in Japanese Patent Application No.
53-80960. A cross section of this apparatus is shown in Fig. 1 of the accompanying drawings.
Referring to Fig. 1, a carrier gas, such as Argon, is introduced into a glass tube 1 through a supply tube 2. One end of the glass tube 1 is closed by an insulating stopper 3, through which a needle-shaped electrode 4 is inserted into the glass tube 1. In said tube 1, a counter electrode 5, which is opposite the electrode 4, a mesh electrode 6, and a repeller electrode 7 are arranged in this order, between which insulating rings 8 and 9 are inserted. An emitter 10 is supported by an insulating base 11 and is inserted into the glass tube 1 through an opening in the side wall of the glass tube 1.
The method of using the apparatus in Fig. 1 comprised the following steps: (a) producing Argon ions (Ar+), electrons (e-) and excited Argon atoms (Ar*: metastable species) by corona discharge between the needle electrode 4 and the counter electrode 5; (b) removing Ar+ and e- by the electrodes 5 and 6; and (c) ionizing a sample on the emitter 10 by the internal energy of Ar*, said energy being thereby transferred to the sample at the time that Ar* contacts the sample.
The following advantages can be realised with this method and apparatus: (a) liquid samples can be directly ionised under atmospheric pressure: (b) by using Argon as the carrier gas, most organic compounds can be ionised; (c) since ionisation is performed under atmospheric pressure, sample handling is easy; and (d) since evacuation is not essential, the structure of the apparatus can be simplified.
When the apparatus is combined with a mass spectrometer, it is necessary to generate a large quantity of sample ions and effectively to introduce them into the mass spectrometer. Therefore, the present inventor has tried to use an FD (Field Desorption) emitter which comprises a wire having a large number of whiskers, as the emitter 1 0. It is not possible, however, to fully satisfy such requirements.
The present invention relates to an improvement over the aforesaid apparatus and method, making it more suitable for use with a mass spectrometer.
According to one aspect of the invention, there is provided apparatus for producing sample ions comprising means for producing metastable species by corona discharge in a carrier gas; a needle-shaped emitter whose pointed end is inserted into the stream of carrier gas, which transports said metstable species; and means for applying high potential to said needle-shaped emitter, wherein sample is arranged at or near to the pointed end of said needle-shaped emitter.
According to another aspect of the invention there is provided apparatus for producing metastable species comprising a cylyndrical electrode having an open end; a needle electrode arranged in said cylindrical electrode so that the pointed end of it is directed to the open end of said cylindrical electrode; means for supplying carrier gas in said cylindrical electrode in order to make the stream flow from said needle electrode to the open end of said cylindrical electrode; and means for applying a high potential between said electrodes in order to generate a corona discharge.
According to another aspect of the invention there is provided a method of producing sample ions consisting in: producing metastable species by corona discharge in a carrier gas; arranging that a sample to be ionised is contacted by the metastable species in the carrier gas; providing a needle-shaped emitter with its pointed end inserted in the stream of carrier gas at or near the sample; and applying high potential to the needle-shaped emitter.
The invention will further be described with reference to Figs. 2 to 5 of the accompanying drawings, of which: Figure 2 is a cross section of one embodiment of the invention; Figure 3 is a cross section of another embodiment of the invention; Figure 4 is a cross section of still another embodiment of the invention; and Figures 5A, 5B, 5C, and 5D are cross sections of another embodiment of the invention.
Referring now to Fig. 2, a cylindrical or barrel-shaped electrode 1 2 has a ground potential.
One end of it is sealed by an insulating cap 1 3 and the other end is inserted into an ionization chamber 1 5 which is walled in by an insulating ring 1 4. A needle electrode 1 7 connected to a voltage source 16, is inserted into said electrode 1 2 through the insulating cap 1 3 and is movable back and forth by rotating the insulating cap 1 3. A carrier gas such as Argon, having atmospheric pressure, is introduced into said electrode 1 2 through an inlet tube 18, flows into the ionisation chamber 1 5 and is exhausted from the chamber 1 5 through the outlet holes 1 9 bored in the insulating ring 1 4.
A sample holder 20 having a heater 21 is inserted into the ionisation chamber 15, and the lower surface S of the holder 20 reaches the stream of the carrier gas. On surface S of the holder 20, a sample as a solution or mixed with a matrix such as glycerol (G) is applied. From the direction opposite the holder 20, a nedle-shaped emitter 22 is inserted into the ionisation chamber 1 5. The pointed end of the emitter 22 contacts the sample on the holder 20 and a high potential is applied to the emitter 22 from a voltage source 23. The emitter 22 can be heated by a surrounding heater 24, and the base part of it is sheathed with an insulating cover 25 together with the heater 24. Beyond the insulating ring 14, a mass spectrometer 32, having lens electrodes 27 and 28, quadrupole electrodes 29, an ion detector 30 and a vacuum pump 31, is attached.A pinhole aperture 34 with a pinhole 33 is employed to enable the difference in pressure between the ionisation chamber 1 5 (atmospheric pressure) and the mass spectrometer 32 (high vacuum) to be maintained. The aperture plate 34 is isolated from the surroundings by the insulating ring 14 and 35, and a suitable potential (15V-20V) is applied from a voltage source 36. An insulating plate 26 having an ion penetration hole is arranged between the holder 20 and the aperture 34.
In the above-described arrangement, a carrier gas, such as Argon, is introduced into the cylindrical electrode 1 2 through the inlet tube 1 8 and flows into the ionisation chamber 1 5.
Passing through the holder 20 and the needle emitter 22, the Argon reaches the aperture plate 34, flows to the outlet holes 19, and is exhausted from the ionisation chamber 1 5. A part of the Argon flows into the mass spectrometer 32 through the pinhole 33.
Now, by applying a negative high potential, for example, ranging from - 1 to - 2 KV, to the needle electrode 17, a corona discharge is continuously generated between the pointed end of the electrode 17 and the cylindrical electrode 12. By said discharge, Ar+, e-, and Ar* which is uncharged, are generated around the pointed end of the electrode 1 7. Said Ar* species is in a metastable state (internal energies: 11.55 eV 11.72 eV) and is long-lived (10-3 sec or more).
Ar+, e-, and Ar*, generated by the corona discharge, are transported by the stream of Argon gas towards the ionisation chamber 15; however, Ar+ and e-, both charged, are attracted to the surrounding electrode 1 2 and removed. As a result, at the open end of the cylindrical electrode 12, only Ar* still exist in the carrier gas. Said Ar* is further transported and reaches the needle emitter 22 to which a sufficiently high potential, such as several hundred volts to over one thousand volts, is applied.
When the Ar* collides with or contacts sample M (on top of emitter 22), then sample M, whose ionisation energy is less than the internal energy of Ar* (11.55 eV or 11.72 eV) is ionised according to the following reaction formulae.
Ar* + MoAr + M + + e~ (1) M+ + + Mo(M + H)+ + (M-H) (2) At* + no (kM+H)+ +(mM-H)- +(n-k-m)M+Ar (3) A part of Ar* is changed to Ar+ by the intense electric field around the pointed end of the emitter 22. Said Ar+ has a sufficiently high energy (15.5 eV) to ionise the water molecules which ordinarily exist in the carrier gas and the ionisation chamber 15, or to ionise matrix G.
Then, cluster ions of water (H2O)nH +or GmH + ions are produced and a part of sample is ionised by the proton transfer reaction with said ions according to the following reaction formulae: Ar*+nGGmH+ (n-m-1)G(G-H)+Ar (4) GmH+ + MeMH + + mG (5) Ar+ + H20oH20+ + Ar (6) H2O+ + H2O(H2O)H+ + OH (7) (H2O)H + + H20 + Are(H20)2H + + Ar (8) (H2O)n1H+ +H2O+Ar(H20)nH+ +Ar (9) (H20)nH+ + MEM + + nH2O (10) Sample ions, produced by the above reactions, can be desorbed from the sample surface soon after their ionisation by the intense electric field around the pointed end of the needle emitter 22 and directed toward the pinhole 33 by the convex lens action of the electric field, and are introduced into the mass spectrometer 32 through the pinhole.
As a result, since sample ions are effectively desorbed from the emitter by the intense electric field, a large quantity of sample ions can be produced. Furthermore, since the sample is ionised in the restricted area, namely, at the pointed end of the emitter 22, it is very easy to find an optimum position for the best transmission of ions produced in said restricted area through the pinhole 33.
When the needle electrode 1 7 is moved forward and the pointed end of it is close to the open end of the cylindrical electrode 12, Ar+ produced in the electrode 12 is not effectively removed and a considerable amount of Ar+ is introduced into the ionisation chamber 1 5. Accordingly, it is possible to mainly ionise the sample by aforesaid proton transfer reactions ((6)--(10)) due to said Ar+.
In the case of nonvolatile samples, it is possible to increase the quantity of the sample ions by heating the emitter 22, thereby heating the sample around it. Heating can be done by the heater 21 through the holder 20 or by both heaters 21 and 24. However, in the case of volatile samples, heating and/or matrix is not required.
The holder 20 and/or the emitter 22 has a shifting and tilting mechanism in order to vary the distance and angle between the holder and emitter.
Fig. 3 shows another embodiment suitable for ionising the gaseous sample. In the figure, an inlet pipe 37 is inserted into the ionisation chamber 1 5. The gaseous sample introduced into said chamber 1 5 through the inlet pipe 37 reaches the pointed end of the emitter 22 and is ionised by Ar* (or cluster ions of water) in accordance with the same procedure described above.
A gas chromatograph mass spectrometer (GC-MS) can be realised by connecting the inlet pipe 37 to the output of a gas chromatograph.
Liquid samples and samples mixed in the liquid matrix, such as liquid paraffin, can also be ionised. Fig. 4 shows another embodiment which is suitable in this case. In the figure, the liquid sample or the sample mixed in the liquid matrix is deposited on the pointed end of the emitter 22 by a microsyringe or other device (not shown) which is inserted into the chamber 1 5 at a right angle or from a suitable angleto the drawing.
In this embodiment, a ring electrode 38 is attached to the open end of the cylindrical electrode 12, between which an insulator 39 is inserted. An appropriate positive potential is applied to said electrode 38 from a voltage source 40. Since the electrode 38 works as a repeller, Ar+ and background ions produced in the cylindrical electrode 1 2 can be significantly reduced. Said ring electrode 38 can be adopted in the other embodiments of the invention.
Figs. 5A and 5B show another embodiment suitable for ionising the liquid sample from a liquid chromatograph. Fig. 5A is an X-X' cross section of Fig. 5B and Fig. 5B is a Y-Y' cross section of Fig. 5A. In the figures, the ionisation chamber 1 5 is walled in by a glass dome 41 which corresponds to the insulating ring 14 in Figs. 2 to 4. Said dome 41 has a top opening 42 and side openings 43, 44 and 45 of the same size. The needle emitter 22 is inserted through the top opening 42 from a suitable angle with the ion path passing through the pinhole 33, and the pointed end of the emitter 22 is arranged opposite to the pinhole 33.The cylindrical electrode 1 2 is inserted into the chamber 1 5 through the side opening 43 so as to aim at the pointed end of the emitter 22. An inlet pipe 46 which is connected to the output of a liquid chromatograph (not shown) is inserted into the chamber 1 5 through the side opening 44 so as to deposit liquid sample from the liquid chromatograph on the pointed end of the emitter 22. Sample overflows run down along the outside wall of the inlet pipe 46 and are drawn off through a drain pipe 47. Argon gas in the ionisation chamber 1 5 is exhausted through an exhaust pipe 48.
By changing the inlet pipe 46 for a sample receiver 49 and inserting said inlet pipe 46 into the chamber 1 5 through the side opening 45 as shown in Fig. 5C, it is also possible to ionise the sample from the liquid chromatograph. The sample receiver 49 is composed of an insulating rod and is used for assisting to deposit the sample on the emitter 22.
Furthermore, by changing the receiver 49 for the sample holder 20 and removing the inlet pipe 46 as shown in Fig. 5D, it is possible to ionise sample on top of the holder 20. In this case, the sample can be deposited on the holder 20 by a microsyringe or other device inserted through the side opening 45, which the operator can observe through the glass dome 41.
In the aforesaid embodiment, positive sample ions are extracted. To obtain negative sample ions, it is necessary to invert the polarity of every voltage source, except the voltage source 16.
To summarise, with the present invention, the sample is effectively onised in the restricted area of the pointed end of the emitter 22, and high densities of sample ions can be obtained.
Moreover, it is possible to effectively converge the sample ions from said restricted area through the pinhole 33. Accordingly, a large quantity of sample ions (10 to 100 times that of the previously proposed method and apparatus) can be introduced into the mass spectrometer.

Claims (11)

1. Apparatus for producing sample ions comprising: means for producing metastable species by corona discharge in a carrier gas; a needle-shaped emitter whose pointed end is inserted into the stream of carrier gas, which transports said metastable species; and means for applying high potential to said needle-shaped emitter, wherein sample is arranged at or near to the pointed end of said needle-shaped emitter.
2. Apparatus as claimed in claim 1, further comprising means for heating said needleshaped emitter.
3. Apparatus as claimed in claims 1 to 2, wherein said sample is deposited on the pointed end of the needle-shaped emitter.
4. Apparatus as claimed in claims 1 to 2, further comprising means for carrying gaseous sample to the pointed end of the needle-shaped emitter.
5. Apparatus as claimed in claims 1 to 2, further comprising a sample holder for arranging the sample adjacent to the pointed end of the needle-shaped emitter.
6. Apparatus as claimed in claim 5, further comprising a liquid chromatograph and means for transporting the output of said liquid chromatograph to the sample holder.
7. Apparatus as claimed in claims 5 and 6, further comprising means for heating said sample holder and means for varying the distance and angle between said holder and the needle-shaped emitter.
8. Apparatus as claimed in claims 1 to 7, further comprising a mass spectrometer for analysing sample ions; and a pinhole aperture for introducing sample ions into said mass spectrometer.
9. Apparatus for producing metastable species comprising: a cylindrical electrode having an open end; a needle electrode arranged in said cylindrical electrode so that the pointed end of it is directed to the open end of said cylindrical electrode; means for supplying carrier gas in said cylindrical electrode in order to make the stream flow from said needle electrode to the open end of said cylindrical electrode; and means for applying a high potential between said electrodes in order to generate a corona discharge.
10. Apparatus as claimed in claim 9, further comprising an additional electrode attached to the open end of the cylindrical electrode with an insulator in between and a voltage source for applying a potential to said additional electrode.
11. A method of producing sample ions consisting in producing metastable species by corona discharge in a carrier gas; arranging that a sample to be ionised is contacted by the metastable species in the carrier gas; providing a needle-shaped emitter with the pointed end inserted in the stream of carrier gas at or near the sample; and applying high potential to the needle-shaped emitter.
1 2. Apparatus for producing sample ions substantially as hereinbefore described with reference to any of Figs. 2 to 5 of the accompanying drawings.
GB08320542A 1982-08-20 1983-07-29 Apparatus for producing sample ions Expired GB2127212B (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP57143255A JPS5936385B2 (en) 1982-08-20 1982-08-20 ion generator
JP57143254A JPS5935347A (en) 1982-08-20 1982-08-20 Ion generator

Publications (3)

Publication Number Publication Date
GB8320542D0 GB8320542D0 (en) 1983-09-01
GB2127212A true GB2127212A (en) 1984-04-04
GB2127212B GB2127212B (en) 1987-08-12

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2183902A (en) * 1985-10-30 1987-06-10 Hitachi Ltd Atmospheric pressure ionization mass spectrometer
WO1993011554A1 (en) * 1991-12-03 1993-06-10 Graseby Dynamics Limited Corona discharge ionisation source
EP1860679A1 (en) * 2006-05-23 2007-11-28 ICT, Integrated Circuit Testing Gesellschaft für Halbleiterprüftechnik Mbh Charged particle beam device with a gas field ion source and a gas supply system
US7429731B1 (en) 2005-05-05 2008-09-30 Science Applications International Corporation Method and device for non-contact sampling and detection

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8123396B1 (en) 2007-05-16 2012-02-28 Science Applications International Corporation Method and means for precision mixing
US8008617B1 (en) 2007-12-28 2011-08-30 Science Applications International Corporation Ion transfer device
US8071957B1 (en) 2009-03-10 2011-12-06 Science Applications International Corporation Soft chemical ionization source

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2183902A (en) * 1985-10-30 1987-06-10 Hitachi Ltd Atmospheric pressure ionization mass spectrometer
US4769540A (en) * 1985-10-30 1988-09-06 Hitachi, Ltd. Atmospheric pressure ionization mass spectrometer
GB2183902B (en) * 1985-10-30 1990-02-14 Hitachi Ltd Atmospheric pressure ionization mass spectrometer
USRE35681E (en) * 1985-10-30 1997-12-02 Hitachi, Ltd. Atmospheric pressure ionization mass spectrometer
WO1993011554A1 (en) * 1991-12-03 1993-06-10 Graseby Dynamics Limited Corona discharge ionisation source
US7429731B1 (en) 2005-05-05 2008-09-30 Science Applications International Corporation Method and device for non-contact sampling and detection
EP1860679A1 (en) * 2006-05-23 2007-11-28 ICT, Integrated Circuit Testing Gesellschaft für Halbleiterprüftechnik Mbh Charged particle beam device with a gas field ion source and a gas supply system
US7692165B2 (en) 2006-05-23 2010-04-06 Ict, Integrated Circuit Testing Gesellschaft Fur Halbleiterpruftechnik Mbh Charged particle beam device with a gas field ion source and a gas supply system

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Publication number Publication date
GB2127212B (en) 1987-08-12
DE3329861A1 (en) 1984-02-23
GB8320542D0 (en) 1983-09-01

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PCNP Patent ceased through non-payment of renewal fee

Effective date: 19930729