1. Field of the Invention
Mass Spectrometers often employ multipole ion guides including collision cells. Ion guides include a plurality of electrodes to which a variety of voltages are applied to contain or move ions radially and/or axially. The present invention relates specifically with apparatuses and methods for moving ions axially by auxiliary rods in multipole ion guides and collision cells.
2. Discussion of the Related Art
In tandem mass spectrometers such as triple stage quadrupole mass spectrometers, and also in other mass spectrometers, gas within the volumes defined by the RF rod sets in ion guides and collision cells improves the sensitivity and mass resolution by a process known as collisional focusing. In such a process, collisions between the gas and the ions cause the velocities of the ions to be reduced, causing the ions to become focused near the axis. However, the slowing of the ions also creates delays in ion transmission through the rod sets, and from one rod set to another. While the focusing is desirable, the slowing of the ions is also accompanied by other undesirable effects.
For example, when a rod set of an ion guide transmits ions from an atmospheric pressure ion source into a mass filter, the gas pressure in the ion guide may be relatively high (e.g. above 5 millitorr for collisional focusing) and collisions with the gas can slow the ions virtually to a stop. Therefore, there is a delay between ions entering the ion guide and the ions reaching the mass filter just downstream. This delay can cause problems in multiple ion monitoring, for example, where several ion intensities are monitored in sequence. If these multiple ions are monitored at a frequency which is faster than the ion transit time through the ion guide, then the fact that at least some of the ions are slowed to a stop has the negative impact of also causing the ions to have a sequence and a reduced rate at which the ions can be detected. The sequence and rate at which the associated data is processed and saved is also affected. In this case the signal from ions entering the ion guide may never reach a steady state. Thus, the measured ion intensity may be too low and may be a function of the measurement time.
Similarly, after product ions have been formed in a collision cell downstream of a first mass filter, for example, the ions may drain slowly out of the collision cell because of their very low velocity after many collisions. The ion clear out time (typically several tens of milliseconds) can cause tailing in the chromatogram and other spurious readings due to interference between adjacent channels when monitoring several parent/fragment pairs in rapid succession. To avoid this, a fairly substantial pause time is needed between measurements. The tailing also requires a similar pause. This required pause time between measurements reduces the productivity of the instrument.
In order to move ions axially through the multipoles forming ion guides and collision cells, it is known that the ions can be moved by segmentation of auxiliary rods and the application of voltages to the segments to create a voltage gradient along a length of the multipoles.
Background information for such a method is described in U.S. Pat. No. 5,847,386, entitled, “Spectrometer With Axial Field,” issued Dec. 8, 1998, to Thompson et al., including the following, “In a mass spectrometer, typically a quadrupole, one of the rod sets is constructed to create an axial field, e.g., a DC axial field, thereon. The axial field can be created by tapering the rods, or arranging the rods at angles with respect to each other, or segmenting the rods, or by providing resistively coated or segmented auxiliary rods, or by providing a set of conductive metal bands spaced along each rod with a resistive coating between the bands, or by forming each rod as a tube with a resistive exterior coating and a conductive inner coating, or by other appropriate methods.”
Background information on another segmented auxiliary rod structure is described in U.S. Pat. No. 5,576,540, entitled, “Mass Spectrometer With Radial Ejection,” to Jolliffe, issued Nov. 19, 1996, including the following, “Each rod 140 is divided into a number of axial segments 140-1 to 140-7, separated by insulators 141 . . . . The voltages on rods 140 create an axial DC field along the central longitudinal axis 142 of the rod set 132.”
Background information on other auxiliary electrode structures can also be found in U.S. Pat. No. 3,147,445 to Wuerker et al., U.S. Pat. No. 6,713,757 to Tanner et al., U.S. Pat. No. 6,909,089 to Londry et al and in U.S. Pat. No. 5,783,824, entitled “Ion Trapping Apparatus,” issued Jul. 21, 1998, to Baba et al.
The U.S. Pat. No. 7,067,802 to Kovtoun teaches an alternative way of forming an axial voltage gradient for moving ions through a multipole by applying a resistive path to an outer surface of the main electrodes of a multipole and applying a DC voltage to the resistive path.
The U.S. Pat. No. 7,084,398 to Loboda et al. teaches a method of selectively axially ejecting ions from a trap. The abstract explains that the method includes “ . . . separating the ions into a first group of ions and a second group of ions by providing an oscillating axial electric field within the rod set to counteract the static axial electric field . . . ”.
Hence, the present invention is directed to auxiliary electrodes that can urge ions axially in ion guides and collision cells. There is a need to provide these auxiliary electrodes at low cost and in a manner that makes it feasible to easily configure the auxiliary electrodes to any shape in order to match curved main electrode sets. Placement of a generally flat or low profile array of finger electrodes on a printed circuit board material enables placement of the auxiliary electrodes formed with these arrays between main RF electrodes in a multipole ion guide or collision cell. The placement can be such that radially inward edges are close to the central axis. Thus, axial voltage gradients created by the voltages applied to the array of finger electrodes can effectively move the ions through the multipole.
Embodiments of the present invention include a mass spectrometer having a multipole ion guide device having an electronic controller and a plurality of main electrodes operably connected to the electronic controller and an RF power source for applying RF voltages in the multipole ion guide device under operation of the electronic controller. The mass spectrometer also has at least one auxiliary electrode connected to a DC voltage source via the controller. Such an auxiliary electrode can be disposed between at least two adjacent ones of the main electrodes. The at least one auxiliary electrode may have electrical elements including at least one array of finger electrodes and a plurality of resistors interconnecting respective finger electrodes of the at least one array. The auxiliary electrode may also include a substrate supporting the finger electrodes and the resistors. The voltage source may apply a static DC voltage to the electrical elements such that the finger electrodes present a monotonically progressive voltage gradient on respective finger electrodes of the array along a length of the auxiliary electrode.
Embodiments of the present invention may also include a mass spectrometer similar to that described above, except that electrical elements include at least one digital to analog converter (DAC) connected to respective finger electrodes of the at least one array of finger electrodes instead of or in addition to the resistors. Also, the DC voltage source may apply one or more DC voltage to the finger electrodes by the at least one DAC for presenting a voltage gradient on the respective finger electrodes of the at least one array along a length of the at least one auxiliary electrode for moving ions axially through the multipole ion guide device of the mass spectrometer. In this arrangement, the at least one DAC may include a programmable logic control that can be dynamically adjusted.
In another example arrangement, embodiments of the present invention may include a method of moving ions through a multipole ion guide device in a mass spectrometer. The method may include disposing an auxiliary electrode comprising a thin plate between adjacent main RF electrodes of the multipole ion guide device. The method may also include applying at least one step-wise monotonic range of voltages in an axial direction by at least one array of finger electrodes disposed on the thin plate of the auxiliary electrode. The method may include applying respective voltages in steps to the finger electrodes through respective resistors, and monotonically moving ions through the multipole ion guide device in the axial direction by the range of voltages.
In still another configuration, embodiments of the present invention may include a method similar to that described above, with the exceptions of applying respective DC voltages to the finger electrodes by one or more computer controlled voltage supply instead of, or in addition to, applying the DC voltages by the resistors. The computer controlled voltage supply may include a DAC.
It is to be understood that embodiments of the present invention may include the auxiliary electrodes that may be applied to the mass spectrometers and methods described above. In a simple form, the embodiments of the present invention may thus include an auxiliary electrode for creating an ion moving axial electric field in a multipole ion guide device of a mass spectrometer. The auxiliary electrode may include at least one substrate for supporting electrical elements of the auxiliary electrode. The at least one substrate may be configured to be positioned between at least two adjacent ones of main electrodes of the multipole ion guide device. The electrical elements may include an array of finger electrodes disposed on the at least one substrate, and static resistors interconnecting respective ones of the finger electrodes for setting up a monotonically progressive voltage gradient in an axial direction of the multipole ion guide device for moving ions axially through the multipole ion guide device. In another simple form, the auxiliary electrode may include at least one DAC instead of or in addition to the resistors, as described above. The at least one DAC may be a dynamically adjustable DAC.
The at least one substrate may include a thin plate. The array of finger electrodes may be disposed on the thin plate. The electrical elements may have a low profile or be integral with the thin plate such that the substrate with the electrical elements form a monolithic unit for positioning between the at least two adjacent electrodes of the multipole ion guide device. In one case, the thin plate may include a printed circuit board material and the array of finger electrodes may include a printed conductive material.
In the description of the invention herein, it is understood that a word appearing in the singular encompasses its plural counterpart, and a word appearing in the plural encompasses its singular counterpart, unless implicitly or explicitly understood or stated otherwise. Furthermore, it is understood that for any given component or embodiment described herein, any of the possible candidates or alternatives listed for that component may generally be used individually or in combination with one another, unless implicitly or explicitly understood or stated otherwise. Additionally, it will be understood that any list of such candidates or alternatives is merely illustrative, not limiting, unless implicitly or explicitly understood or stated otherwise. It is also to be understood, where appropriate, like reference numerals may refer to corresponding parts throughout the several views of the drawings for simplicity of understanding.
Moreover, unless otherwise indicated, numbers expressing quantities of ingredients, constituents, reaction conditions and so forth used in the specification and claims are to be understood as being modified by the term “about.” Accordingly, unless indicated to the contrary, the numerical parameters set forth in the specification and attached claims are approximations that may vary depending upon the desired properties sought to be obtained by the subject matter presented herein. At the very least, and not as an attempt to limit the application of the doctrine of equivalents to the scope of the claims, each numerical parameter should at least be construed in light of the number of reported significant digits and by applying ordinary rounding techniques. Notwithstanding that the numerical ranges and parameters setting forth the broad scope of the subject matter presented herein are approximations, the numerical values set forth in the specific examples are reported as precisely as possible. Any numerical values, however, inherently contain certain errors necessarily resulting from the standard deviation found in their respective testing measurements.
Turning now to the drawings,
In other example arrangements, mass spectrometer 12 often may be configured with an ion source and an inlet section 24 known and understood to those of ordinary skill in the art, of which, such sections can include, but are not limited to, electrospray ionization, chemical ionization, thermal ionization, and matrix assisted laser desorbtion ionization sections. In addition, mass spectrometer 12 may also include any number of ion guides (q0) 27, (q4) 30, mass filters (Q1) 33, collision cells (q2) 36, and/or mass analyzers (Q3) 39, (Qn) 42, wherein the mass analyzers 39, 42, may be of any type, including, but not limited to, quadrupole mass analyzers, two dimensional ion traps, three dimensional ion traps, electrostatic traps, and/or Fourier Transform Ion Cyclotron Resonance analyzers.
The ion guides 27, 30, collision cells 36, and analyzers 39, 42, as known to those of ordinary skill in the art, can form an ion path 45 from the inlet section 24 to at least one detector 48. Any number of vacuum stages may be implemented to enclose and maintain any of the devices along the ion path at a lower than atmospheric pressure. The electronic controller 15 is operably coupled to the various devices including the pumps, sensors, ion source, ion guides, collision cells and detectors to control the devices and conditions at the various locations throughout the mass spectrometer 12, as well as to receive and send signals representing the particles being analyzed.
As described above, many ion guides and collision cells suffer from the trade off of slowing the ions down during ion transport when a gas is used to cool the ions and move them toward a central axis. Various mechanisms have been utilized to urge the ions along the ion path 45, as shown in
Turning back to
In an alternative embodiment, as shown in
As shown in
A structural element for receiving and supporting metallization may be a substrate 99, as shown in
In the end view perspective of
As may be appreciated from
As with the other example embodiments, the array of finger electrodes 128 is disposed on opposite sides of the circuit board material that forms each of the substrates 116, 117, 118, 119. Similar to the other example embodiments described above, the array of finger electrodes 128 may include a printed or otherwise applied conductive material on an edge of the printed circuit board material that joins the conductive material on opposite sides of the circuit board material. In this way, the array of finger electrodes presents the conductive material on a majority of a radially innermost edge surface of the auxiliary electrode. Also similar to the other embodiments, there are recesses 92 in the edges of the circuit board material between respective finger electrodes 128 of the finger electrode array. Thus, available sites for ion deposit on an insulative material surface of the circuit board material are recessed radially outward away from the ion beam or path.
As with the other embodiments, the printed circuit board material utilized in forming the auxiliary electrodes for the embodiment of
In all of the embodiments, the auxiliary electrodes may be applied to less than an entire length of a multipole device. While a monotonically progressive change in voltages along a length of the auxiliary electrodes has been discussed, it is to be understood that other non-monotonically progressive changes in voltages may be applied. For example, slowing voltages may be applied in an upstream end of the multipole device such that less collision gas is needed in a collision cell. Then, accelerating voltages may be applied in a downstream end of the multipole device to keep the ions moving through and out of the device. Additionally, DACs or other computer controlled voltage supplies may be utilized to dynamically vary voltages applied to the auxiliary electrodes in place of or in addition to static DC voltage supplies.
It is to be understood that a mass spectrometer can function with only one auxiliary electrode inserted between any adjacent pair of main RF electrodes. However, a more evenly distributed axial DC field is created by a plurality of auxiliary electrodes disposed between respective pairs of adjacent main RF electrodes in the multipole device of any of the embodiments disclosed herein. This is especially so when the same or similar voltage gradient is created in each of the auxiliary electrodes along respective lengths of the auxiliary electrodes.
Number | Name | Date | Kind |
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3147445 | Wuerker et al. | Sep 1964 | A |
5576540 | Jolliffe | Nov 1996 | A |
5679950 | Baba et al. | Oct 1997 | A |
5783824 | Baba et al. | Jul 1998 | A |
5847386 | Thomson et al. | Dec 1998 | A |
6403955 | Senko | Jun 2002 | B1 |
6713757 | Tanner et al. | Mar 2004 | B2 |
6791078 | Giles et al. | Sep 2004 | B2 |
6800846 | Bateman et al. | Oct 2004 | B2 |
6884995 | Bateman et al. | Apr 2005 | B2 |
6909089 | Londry et al. | Jun 2005 | B2 |
6914241 | Giles et al. | Jul 2005 | B2 |
7067802 | Kovtoun | Jun 2006 | B1 |
7084398 | Loboda et al. | Aug 2006 | B2 |
7095013 | Bateman et al. | Aug 2006 | B2 |
7196324 | Verentchikov | Mar 2007 | B2 |
7365317 | Whitehouse et al. | Apr 2008 | B2 |
20070278397 | Bateman et al. | Dec 2007 | A1 |
20090302209 | Green et al. | Dec 2009 | A1 |
Number | Date | Country |
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0290712 | Nov 1990 | EP |
Number | Date | Country | |
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20090294641 A1 | Dec 2009 | US |