LOW PRESSURE ELECTROSPRAY IONIZATION SYSTEM AND PROCESS FOR EFFECTIVE TRANSMISSION OF IONS

Abstract

A system and method are disclosed that provide up to complete transmission of ions between coupled stages with low effective ion losses. A novel “interfaceless” electrospray ionization system is further described that operates the electrospray at a reduced pressure such that standard electrospray sample solutions can be directly sprayed into an electrodynamic ion funnel which provides ion focusing and transmission of ions into a mass analyzer.

Description

FIELD OF THE INVENTION

The present invention relates generally to analytical instrumentation and more particularly to a low pressure electrospray ionization system and process for effective transmission of ions between coupled ion stages with low ion losses.

BACKGROUND OF THE INVENTION

Achieving high sensitivity in mass spectrometry (MS) is key to effective analysis of complex chemical and biological samples. Every significant improvement in MS detection limits will enable applications that are otherwise impractical. Advances in MS sensitivity can also increase the dynamic range over which quantitative measurements can be performed.

FIG. 1 illustrates an electrospray ionization/mass spectrometer (ESI/MS) instrument configuration of a conventional design. In the figure, an atmospheric pressure electrospray ionization (ESI) source with an ES emitter couples to an ion funnel positioned in a low pressure (e.g., 18 Torr) region via a heated inlet capillary interface. Ions formed from electrospray at atmospheric pressure are introduced into the low pressure region through the capillary inlet and focused by the first ion funnel. A second ion funnel operating at a lower pressure (e.g., 2 Torr) than the first ion funnel operating pressure provides further focusing of ions prior to their introduction into a mass analyzer.

It well known in the art that sensitivity losses in ESI/MS are pronounced at the interface between the atmospheric pressure region and the low pressure region. Ion transmission through conventional interfaces is essentially limited by small MS sampling inlets—typically between 400 μm to 600 μm in diameter—required to maintain a good vacuum pressure in the MS analyzer. Sampling inlets can account for up to 99% of ion losses in the interface region, providing less than about 1% overall ion transmission efficiency. Accordingly, new systems, devices, and methods are needed to effectively eliminate the major ion losses in interface regions, e.g., between atmospheric ion source stage and a subsequent low pressure stage important to sensitive ion analyses.

SUMMARY OF THE INVENTION

The invention is an electrospray ionization source that includes an electrospray emitter (transmitter) positioned in a direct ion transfer relationship with an entrance (receiving) aperture of a first ion guide (e.g., electrodynamic ion funnel or multipole ion guide). The ion plume formed by the electrospray is transmitted to and received by the first ion guide with low effective ion losses.

The invention further includes a method for introducing ions into a low pressure environment. The method includes: providing an electrospray ionization source that includes an electrospray emitter (transmitter) positioned in a direct relationship with a entrance aperture of a first ion guide; discharging a preselected quantity of analyte ions or material through the electrospray transmitter in a plume, such that a preselected portion of the plume is received within the first ion guide with low effective ion losses.

The invention is further a system for introducing ions into a low pressure environment. An electrospray emitter (transmitter) is positioned in a direct relationship at the entrance aperture of a first ion guide in a reduced atmosphere (pressure) environment. A preselected portion of an ion plume emitted by the electrospray transmitter is received within the ion guide with low effective ion losses. The preselected portion of the ion plume received by the first ion guide is transmitted to the next ion guide in a further reduced pressure environment with low effective ion losses.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 (Prior Art) illustrates an ESI/MS instrument configuration of a conventional design.

FIGS. 2 a-2d illustrate various embodiments of the present invention.

FIGS. 3 a-3b present mass spectra resulting from a calibration solution infused (a) through a conventional atmospheric pressure ESI emitter and heated inlet capillary interface, and (b) through a low pressure ESI emitter of the invention.

FIGS. 4 a-4c present mass spectra resulting from a reserpine solution (a) infused through a conventional atmospheric pressure ESI emitter and heated inlet capillary interface, (b) infused through a low pressure ESI emitter of the invention, and (c) analyzed with RF voltage to a first ion funnel turned off.

FIG. 5 plots ES current across an ion plume as a function of different ES chamber pressures.

FIG. 6 plots peak intensity as a function of RF voltage for a reserpine solution analyzed with the preferred embodiment of the invention.

FIG. 7 plots peak intensity as a function of flow rate at fixed RF voltage for a reserpine solution, analyzed with the preferred embodiment of the invention.

FIG. 8 plots transmission curves for leucine, enkephalin, reserpine, bradykinin and ubiquitin ions as a function of pressure, analyzed with the preferred embodiment of the invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT OF THE INVENTION

While the present disclosure is exemplified by a description of the preferred embodiments, it should be understood that the invention is not limited thereto, and variations in form and detail may be made without departing from the scope of the invention. All modifications as would be envisioned by those of skill in the art in view of the disclosure are within the scope of the invention.

FIG. 2 a illustrates an instrument system 100 of the invention incorporating a preferred embodiment of an ESI source emitter 10. ES emitter (transmitter) 10 is shown positioned in a direct relationship with a first ion guide 20a, in this case an electrodynamic ion funnel 20a, via a receiving (entrance) aperture, in this case the first electrode of the electrodynamic ion funnel. ES emitter 10 was placed inside a first vacuum region 50 and positioned at the entrance of the first electrodynamic ion funnel, allowing the entire ES plume to be sampled by (i.e., transmitted directly to or within) the ion funnel. A second ion funnel 30a is shown within a second reduced pressure region or environment 60 to effect ion focusing prior to introduction to the vacuum region 70 of a mass selective analyzer 40. The second ion funnel is coupled to the first ion funnel. In the instant configuration, mass spectrometer 40 is preferably a single quadrupole mass spectrometer, but is not limited thereto. First ion funnel 20a had a lower capacitance than second ion funnel 30a, as described, e.g., by Ibrahim et al. (in J. Am. Soc. Mass Spectrom. 2006, 17, 1299-1305, incorporated herein in its entirety), but is not limited thereto. The low capacitance ion funnel permits use of higher frequency and amplitude RF voltage to effect capture and transmission of the ES ion plume for desolvation of the analyte at higher relative pressure compared to pressure in second ion funnel chamber 60. Transmission of ions in the ion plume from emitter 10 to first ion funnel 20a, to second ion funnel 30a, and ultimately to vacuum 70 of mass analyzer 40 occurs with low ion losses. In particular, transmission of ions in the ion plume proceeds at efficiencies or quantities up to 100%. And, results from test experiments demonstrated ion losses were significantly reduced compared to a conventional atmospheric pressure ESI source and heated capillary interface. Experiments further demonstrated that stable electrosprays were achieved at pressures down to at least about 25 Torr in pressure region 50.

Pressures described in conjunction with the instant embodiment are not to be considered limiting. In particular, pressures may be selected below atmospheric pressure. More particularly, pressures may be selected in the range from about 100 Torr to about 1 Torr. Most particularly, pressures may be selected below about 30 Torr. Thus, no limitations are intended.

While the instant embodiment has been described with reference to a single ES emitter, the invention is not limited thereto. For example, the emitter can be a multiemitter, e.g., as an array of emitters. Thus, no limitations are intended.

FIG. 2 b illustrates an instrument system 200, according to another embodiment of the invention. In the instant configuration, the second ion funnel (FIG. 2a) is replaced by (exchanged with) an RF multipole ion guide 30b. Here, other illustrated components (emitter 10 and first ion funnel 20b) and pressures (e.g. in regions 50, 60, and 70) are identical to those previously described in reference to FIG. 2a, but should not be considered limiting. Multipole ion guide 30b can include (2·n) poles to effectively focus and transmit ions into MS 40, where n is an integer greater than or equal to 2. No limitations are intended.

FIG. 2 c illustrates an instrument system 300, according to yet another embodiment of the invention. In system 300, the first ion funnel (FIG. 2a) is replaced by an RF multipole ion guide 20c, which can include (2·n) poles to effectively focus and transmit ions into second ion funnel 30c, where n is any integer greater than 1. To effectively capture the ES plume, each pole in the multipole ion guide 20c can be tilted with a uniform or non uniform angle to create a larger entrance aperture facing the ES plume, and a smaller exit aperture into the second ion funnel. No limitations are intended. Other illustrated components (emitter 10 and MS 40) and pressures (e.g. in regions 50, 60, and 70) are identical to those previously described in reference to FIG. 2a, but should not be considered limiting.

FIG. 2 d illustrates an instrument system 400 according to still yet another embodiment of the invention. In the instant system, both the first ion funnel and the second ion funnel (FIG. 2a) described previously are replaced by two RF multipole ion guides 20d and 30d, respectively. Multipole ion guides 20d and 30d can include (2.n) poles to effectively focus and transmit ions, where n is any integer greater than 1. Each pole in multipole ion guide 20d can be tilted with a uniform or non uniform angle to create a larger entrance aperture facing the ES plume, and a smaller exit aperture. Other illustrated components (emitter 10 and MS 40) and pressures (e.g. in regions 50, 60, and 70) are identical to those previously described in reference to FIG. 2a, but should not be considered limiting. For example, as will be understood by those of skill in the art, multipole ion guides described herein can be further replaced with segmented multipole ion guides. Thus, no limitations should be interpreted by the description to present components. An electric field along the axis of the selected ion guide can be created by applying a DC potential gradient to different segments of the ion guide to rapidly push ions through the ion guide.

In a test configuration of the preferred embodiment of the invention (FIG. 2a), emitter 10 was a chemically etched capillary emitter, prepared as described by Kelly et al. (in Anal. Chem. 2006, 78, 7796-7801) from 10 μm I.D., 150 μm O.D. fused silica capillary tubing (Polymicro Technologies, Phoenix, Ariz., USA). The ES emitter was coupled to a transfer capillary and a 100 μL syringe (Hamilton, Las Vegas, Nev., USA) by a stainless steel union, which also served as the connection point for the ES voltage. Analyte solutions were infused from a syringe pump (e.g., a model 22 syringe pump, Harvard Apparatus, Inc., Holliston, Mass., USA). Voltages were applied to the ES emitter via a high voltage power supply (e.g., a Bertan model 205B-03R high voltage power supply, Hicksville, N.Y., USA). A CCD camera with a microscope lens (Edmund Optics, Barrington, N.J.) was used to observe the ES. Placement of the ES emitter was controlled by a mechanical vacuum feedthrough (Newport Corp., Irvine, Calif., USA). A stainless steel chamber was constructed to accommodate placement of the ES emitter at the entrance of the first ion funnel. The chamber used three glass windows, one at the top of the chamber, and one on each side of the chamber that allowed proper lighting for visual observation of the ES by the CCD camera. An ion funnel consisting of seventy (70) electrodes was used to allow the ES emitter to be observed through the viewing windows. A grid electrode (FIG. 2a) was made from a ˜8 line-per-cm mesh rated at 93.1% transmission and placed 0.5 mm in front of the first ion funnel as a counter electrode for the ES, biased to 450 V. The ES emitter was placed ˜5 mm in front of the grid electrode and centered on axis with the ion funnel. The vacuum chamber contained feedthroughs for the ES voltage, an infusion capillary, and a gas line controlled by a leak valve to room air. A rough pump (e.g., a model E1M18 pump, BOC Edwards, Wilmington, Mass., USA) was used to pump the chamber. The pumping speed was regulated by an in-line valve. A gate valve was built into the first ion funnel and was located between the last ion funnel RF/DC electrode plate and the conductance limiting orifice plate, allowing ES chamber venting and ES emitter maintenance without having to vent the entire mass spectrometer. The gate valve was constructed from a small strip of 0.5 mm thick TEFLON®, which was placed between the last ion funnel electrode and the conductance limiting orifice electrode and attached to an in-house built mechanical feedthrough, which moved the TEFLON® over the conductance limiting orifice during venting of the ES chamber. For all atmospheric pressure ESI experiments, a conventional configuration (FIG. 1) was used for comparison purposes, comprising a 6.4 cm long, 420 μm I.D. inlet capillary heated to 120° C. that terminated flush with the first electrode of the first ion funnel. The atmospheric pressure ESI source and ES emitter were controlled using a standard X-Y stage (e.g., a Model 433 translation stage, Newport Corp., Irvine, Calif., USA).

In the test configurations of FIG. 1 and FIG. 2a, a low capacitance ion funnel, e.g., as described by Y. Ibrahim et al. (in J. Am. Soc. Mass Spectrom. 2006, 17, 1299-1305, incorporated herein in its entirety) was used that could be effectively operated at higher pressure. In the test configuration of FIG. 1, to maintain high ion transmission efficiency at high pressure, both the funnel RF frequency and amplitude were raised from typical operating frequencies and amplitudes of 550 kHz and 80 V_p-p to 1.3 MHz and 175 V_p-p, respectively. The first ion funnel consisted of 100, 0.5 mm thick ring electrode plates separated by 0.5 mm thick TEFLON® insulators. A front straight section of the ion funnel consisted of 58 electrodes with a 25.4 mm I.D. The tapered section of the ion funnel included 42 electrodes that linearly decreased in I.D., beginning at 25.4 mm and ending at 2.5 mm. A jet disrupter electrode described, e.g., by J. S. Page et al. (in J. Am. Soc. Mass Spectrom. 2005, 16, 244-253) was placed 2 cm down from the first ion funnel plate and biased to 380 V. The last electrode plate was a DC-only conductance limiting orifice with a 1.5 mm I.D. biased to 210 V. Excess metal was removed from the electrode plates to reduce capacitance, enabling greater RF frequencies and voltages. In the test configuration of FIG. 2a, the first ion funnel was otherwise identical to that in test configuration FIG. 1 except that 30 funnel electrodes were removed from the straight section, leaving a total of 28 electrodes with a 25.4 mm I.D. in the straight section of the ion funnel. A 1.3 MHz RF with an amplitude of 350 V_P-P was used. No jet disrupter was used for the first ion funnel in the test configuration of FIG. 2a. The first ion funnels in both test configurations of FIG. 1 and FIG. 2a had the same DC voltage gradient of 18.5 V/cm. The second ion funnel was identical to the first ion funnel in FIG. 1 and used in a subsequent vacuum region for both the test configurations of FIG. 1 and FIG. 2a. A 740 kHz RF with amplitude of 70 V_P-P was applied to the second ion funnel along with a DC voltage gradient of 18.5 V/cm. The jet disrupter and 2.0 mm I.D. conductance limiting orifice were biased to 170 V and 5 V, respectively. An Agilent MSD1100 (Santa Clara, Calif.) single quadrupole mass spectrometer was coupled to the dual ion funnel interface, and ultimately to the ESI ion source and emitter. Mass spectra were acquired with a 0.1 m/z step size. Each spectrum was produced from an average of 10 scans to reduce effects of any intensity fluctuations in the ES.

In the test configuration, a linear array of (23) electrodes was incorporated into the front section of a heated capillary assembly, described, e.g., by J. S. Page et al. (in J. Am. Soc. Mass Spectrom. 2007, in press) to profile the ES current lost on the front surface of the entrance aperture at various ES chamber pressures. A 490 μm id, 6.4 cm long, stainless steel capillary was silver soldered in the center of a stainless steel body. Metal immediately below the entrance aperture was removed and a small stainless steel vice was constructed on the entrance aperture to press 23 KAPTON®-coated 340 μm O.D. copper wires in a line directly below the aperture entrance. The front of the entrance aperture was machined flat and polished with 2000 grit sandpaper (Norton Abrasives, Worcester, Mass.) making the ends of the wires an array of round, electrically isolated electrodes each with diameter of 340 μm. The other ends of the wires were connected to an electrical breadboard with one connection to common ground and another to a picoammeter (e.g., a Keithley model 6485 picoammeter, Keithley, Cleveland, Ohio) referenced to ground. The electrode array was used as the inlet to the single quadrupole mass spectrometer and installed inside the ES vacuum chamber. ES current was profiled by sequentially detecting current on all 23 electrodes by selecting and manually moving the appropriate wire from the common ground output to the picoammeter input and acquiring 100 consecutive measurements. Measurements were averaged using the data acquisition capabilities of the picoammeter. A further understanding of the preferred embodiment of the ES source and emitter of the invention will follow from Examples presented hereafter.

EXAMPLE 1

Testing of Low Pressure ESI Source and Emitter

The low pressure ESI source and emitter of the preferred embodiment of the invention was tested by analyzing 1) a calibration (calibrant) solution (Product No. G2421A, Agilent Technologies, Santa Clara, Calif., USA) containing a mixture of betaine and substituted triazatriphosphorines dissolved in acetonitrile and 2) a reserpine solution (Sigma-Aldrich, St. Louis, Mo., USA). A methanol:water solvent mixture for ESI was prepared by combining purified water (Barnstead Nanopure Infinity system, Dubuque, Iowa) with methanol (HPLC grade, Fisher Scientific, Fair Lawn, N.J., USA) in a 1:1 ratio and adding acetic acid (Sigma-Aldrich, St. Louis, Mo., USA) at 1% v/v. A reserpine stock solution was also prepared in a n-propanol:water solution by combining n-propanol (Fisher Scientific, Hampton, N.H., USA) and purified water in a 1:1 ratio and then diluting the ES solvent to a final concentration of 1 μM. Respective solutions were then electrosprayed: A) using conventional atmospheric pressure ESI with the heated inlet capillary (see FIG. 1) and B) using the low pressure ESI source in which the ES emitter was placed at the entrance aperture of the first ion funnel (FIG. 2a) in the first low vacuum pressure region at 25 Torr. FIGS. 3a-3b present mass spectra obtained with respective instrument configurations from analyses of the calibration solution infused at 300 nL/min. FIGS. 4a-4c present mass spectra obtained with respective instrument configurations from analyses of a 1 μM reserpine solution infused at 300 nL/min. In FIG. 4c, the spectrum was acquired with RF voltage to the first ion funnel turned off, which greatly reduced ion transmission and showed utility of the ion guide in the preferred embodiment of the invention.

A comparison of results from analysis of the calibration solution using the test configuration with the low pressure ESI source of the preferred embodiment of the invention (FIG. 2a) and the conventional atmospheric ESI (FIG. 1) in FIGS. 3a and 3b showed a 4- to 5-fold improvement in sensitivity when ES was performed using the low pressure ESI source. In FIG. 4b, a sensitivity increase of ˜3 fold for reserpine is obtained over that obtained in FIG. 4a. In the preferred configuration, the emitter was positioned so that the ion/charged droplet plume was electrosprayed directly into the first ion funnel. Both the emitter and ion funnel were in a 25 Torr pressure environment. Results indicate that removing the conventional capillary inlet and electrospraying directly into an ion funnel can decrease analyte loss in an ESI interface. In FIG. 4c, turning off the RF voltage of the first ion funnel eliminates ion focusing in this (ion funnel) stage, greatly reducing focusing and thus transmission of ions to subsequent stages and to the mass spectrometer. Results demonstrate need for the ion funnel, which effectively transmits ES current into the second ion funnel.

In these spectra, in addition to reserpine peaks, there is also an increase in lower mass background peaks which correspond to singly charged ion species, but do not correspond to typical reserpine fragments. Origin of these peaks is unclear, but may be evidence of clusters of solvent species or impurities.

In these figures, reduction in analyte losses using the low pressure ESI source of the preferred embodiment of the invention yields corresponding increases in ion sensitivity, a consequence of removing the requirement for ion transmission through a metal capillary.

EXAMPLE 2

ES Current Profiling

The ES current was profiled at various chamber pressures using a linear array of charge collectors positioned on the mass spectrometer inlet. Pressures ranged from atmospheric pressure (e.g., 760 Torr) to 25 Torr. Current was measured using a special counter electrode array positioned 3 mm from the ESI emitter, which provided a profile, or slice, of the ES current at the center of the ion/charged droplet plume. The solvent mixture electrosprayed by the ESI emitter consisted of a 50:50 methanol:water solution with 1% v/v acetic acid, which was infused to the ES emitter at a flow rate of 300 nL/min. Utility of an electrode array in the characterization of electrosprays is described, e.g., by J. S. Page et al. (in J. Am. Soc. Mass Spectrom. 2007, in press). FIG. 5 plots the radial electric current distribution of the electrospray plume as a function of pressure.

In the figure, a stable ESI current of 42 nA was achieved at the selected (300 nL/min) flow rate, which can be maintained in a broad range of pressures by simply adjusting the spray voltage. As shown in FIG. 5, a well behaved electrospray is evident for pressures as low as 25 Torr. Higher pressures produced a plume that was ˜5 mm wide. At 100 Torr and 50 Torr, the plume narrowed slightly with an increase ES current density and this was more pronounced at 25 Torr. ES flow rate, voltage, and current changed minimally as pressure was lowered. Decrease in the spray plume angle at lower pressures may be a consequence of narrower ion/droplet plumes detected by the electrode array. Results are attributed to an increase in electrical mobility as a result of an increase in mean-free-path, described, e.g., by Gamero-Castano et al. (in J. Appl. Phys. 1998, 83, 2428-2434). Another observation was the independence of the electrospray (ES) on pressure, which has been described, e.g., Aguirre-de-Carcer et al. (in J. Colloid Interface Sci. 1995, 171, 512-517). Profiling of the ES current detected the charge distribution across the ion/charged droplet plume, but did not provide information on the creation (ionization) of liberated, gas-phase, ions, i.e., the “ionization efficiency”. Ionization efficiency is described further hereafter.

EXAMPLE 3

Ionization Efficiency

In order to investigate ionization efficiency, the low pressure ES source was coupled to a single quadrupole mass spectrometer. Baseline measurements of a reserpine and calibration solution prepared as in Example 1 were first acquired using a standard atmospheric ESI source with a heated metal inlet capillary (FIG. 1). The test configuration used two ion funnels. The front ion funnel operated at 18 Torr; back ion funnel operated at 2 Torr. Similar transmission efficiencies were obtained to those described, e.g., Ibrahim, et al. (in J. Am. Soc. Mass Spectr. 2006, 17, 1299-1305) for single ion funnel interfaces, while allowing a much larger sampling efficiency (i.e., inlet conductance).

EXAMPLE 4

Effect of Varying RF Voltage on Analyte Declustering/Desolvation

Importance of declustering/desolvation and transmission in the low pressure ESI source configuration of the invention was further investigated by varying RF voltage. Ion funnels have been shown to impart energy to analyte ions by RF heating, described, e.g., by Moision et al. (in J. Am. Soc. Mass Spectrom. 2007, 18, 1124-1134). The greater the RF voltage, the greater the amount of energy conveyed to ions/clusters, which can aid desolvation and declustering. FIG. 6 is a plot of reserpine intensity versus the amplitude of RF voltage applied to the first ion funnel. In the figure, error bars indicate the variance in three replicate measurements. Peak intensity quickly rises as the voltage is increased and begins to level off around 300 V_P-P, indicating that adding energy to the ions/clusters liberates more reserpine ions. Increasing voltage also increases the effective potential of the ion funnel, which may provide better focusing of droplets and larger clusters contributing to increased sensitivity.

As will be appreciated by those of skill in the art, components in the instrument configurations described herein are not limited. For example, as described hereinabove, the first ion funnel can be used as a desolvation stage for removing solvent from analytes of interest. Desolvation may be further promoted, e.g., in conjunction with heating of the emitter and/or other instrument components using a coupled heat source, including, but not limited to, e.g., heated gases and sources, radiation heat sources, RF heat sources, microwave heat sources, radiation heat sources, inductive heat sources, heat tape, and the like, and combinations thereof. Additional components may likewise be used as will be selected by those of skill in the art. Thus, no limitations are intended.

EXAMPLE 5

Effect of Fixed RF Voltage and Varying Flow Rates on Analyte Desolvation

Analyte desolvation was further explored by changing solution flow rates and keeping RF voltage fixed at 350 V_P-P. To determine if smaller droplets improve desolvation in the low pressure ESI source of the invention, reserpine solution was infused at flow rates ranging from 50 nL/min to 500 nL/min. FIG. 7 plots peak intensity for reserpine, with error bars corresponding to three replicate measurements. In the figure, peak intensity decreases initially as flow rate is lowered from 500 nL/min to 300 nL/min, and begins to decrease more slowly at the lower flow rates. Results indicate that even though less reserpine is delivered to the ES emitter at lower flow rates, a greater percentage of reserpine is converted to liberated ions. Results demonstrate 1) that the ion funnel effectively desolvates smaller droplets, and 2) that improved desolvation is needed at higher flow rates.

ES droplet size correlates with the flow rate, as described, e.g., by Wilm et al. (in Int. J. Mass Spectrom. Ion Processes 1994, 136, 167-180) and Fernandez de la Mora et al. (in J. Fluid Mech. 1994, 155-184). Smaller flow rates thus create smaller droplets, and smaller droplets require less desolvation and fission events to produce liberated analyte ions.

EXAMPLE 6

Ion Transmission Efficiency

Transmission efficiency of ions in an ion funnel was tested as a function of pressure by analyzing ions having different mass-to-charge ratios. Ions included Leucine, Enkephalin, Reserpine, Bradykinin, and Ubiquitin. The first ion funnel was operated with RF 1.74 MHz and amplitude ranging from 40 to 170 V_p-p. The second ion funnel was operated at RF 560 kHz and 70 V_p-p. FIG. 8 presents experimental results.

In the figure, data for Bradykinin represent the sum of 2+ charge states. Data for Ubiquitin represent the sum of charge states up to 12+. Each dataset is normalized to its own high intensity point. Ion transmission efficiency remains approximately constant up to a 30 Torr pressure maximum. Overlapping operating pressure between the low pressure electrospray and the high pressure ion funnel makes it possible to couple them directly without the need of an inlet orifice/capillary. Results demonstrate that stable electrospray can be maintained at pressures as low as 25 Torr and that good ion transmission can be obtained in the high pressure ion funnel at pressures as high as 30 Torr. Overlap between the two pressures indicates that the concept of interfaceless ion transmission in the instrument is practical. Results further indicate that biological analyses in conjunction with the invention are conceivable and may ultimately prove to be an enabling technology applicable to high-throughput proteomics analyses. The invention could thus prove to be a significant breakthrough in reducing ion losses from electrospray ionization, which along with MALDI, is a prevalent form of ionizing biological samples for analysis by mass spectrometry.

Results presented herein are an initial demonstration of an ESI source/ion funnel combination for producing and transmitting ions in a low pressure (e.g., 25 Torr) environment for use in MS instruments. Use of the ion funnel or other alternatives as illustrated in FIG. 2 is critical to the success of the low pressure ESI source. A large (˜2.5 cm), entrance I.D. provides sufficient acceptance area for an entire ES plume to be sampled into the ion funnel device. In addition, the length of the ion funnel and the RF field employed therein provide a region for desolvation prior to transmission into the mass spectrometer. Sensitivity gains were observed for all solutions analyzed.

While an exemplary embodiment of the present invention has been shown and described, it will be apparent to those skilled in the art that many changes and modifications may be made without departing from the invention in its true scope and broader aspects. The appended claims are therefore intended to cover all such changes and modifications as fall within the spirit and scope of the invention.

Claims

1. An electrospray ionization source, comprising: an electrospray transmitter positioned in a direct relationship with a receiving aperture of a first electrodynamic ion funnel;whereby a preselected portion of a plume emanating from said electrospray transmitter is received within said first electrodynamic ion funnel.

2. The electrospray ionization source of claim 1, wherein said transmitter is a single emitter.

3. The electrospray ionization source of claim 1, wherein said transmitter is a multi emitter.

4. The electrospray ionization source of claim 1, wherein said first electrodynamic ion funnel is exchanged with a tilted RF multipole ion guide configured with a larger receiving aperture and a smaller exit aperture.

5. The electrospray ionization source of claim 4, wherein said tilted RF multipole ion guide comprises 2n poles, where n is an integer greater than or equal to 2.

6. The electrospray ionization source of claim 4, wherein said tilted RF multipole ion guide is exchanged with a tilted segmented RF multipole ion guide.

7. The electrospray ionization source of claim 1, wherein said electrospray ionization source is located within a first vacuum region.

8. The electrospray ionization source of claim 1, wherein said electrospray transmitter is positioned within a first vacuum region having a pressure less than about 30 Torr.

9. The electrospray ionization source of claim 1, further comprising a second electrodynamic ion funnel.

10. The electrospray ionization source of claim 9, wherein said second electrodynamic ion funnel is exchanged with an RF multipole ion guide.

11. The electrospray ionization source of claim 10, wherein said RF multipole ion guide comprises 2n poles, where n is an integer greater than or equal to 2.

12. The electrospray ionization source of claim 10, wherein said RF multipole ion guide is exchanged with a segmented RF multipole ion guide.

13. The electrospray ionization source of claim 1, further comprising a second vacuum region.

14. The electrospray ionization source of claim 1, wherein said electrospray transmitter is located at the entrance of the receiving aperture of said first electrodynamic ion funnel.

15. The electrospray ionization source of claim 1, wherein said electrospray transmitter is located within the receiving aperture of said first electrodynamic ion funnel.

16. The electrospray ionization source of claim 1, wherein said electrospray transmitter is positioned at a preselected distance from said first electrodynamic ion funnel, whereby entire plume is captured within said first electrodynamic ion funnel.

17. The electrospray ionization source of claim 1, further comprising a heat source.

18. A method for introducing ions into a low pressure environment, comprising the steps of: providing an electrospray ionization source comprising an electrospray transmitter positioned in a direct relationship with a receiving aperture of a first electrodynamic ion funnel;discharging a preselected quantity of an analyte material through said electrospray transmitter; andwhereby a preselected portion of a plume emanating from said electrospray transmitter is received within said first electrodynamic ion funnel.

19. A system for introducing ions into a low pressure environment comprising: at least one electrodynamic ion funnel having a receiving aperture, said at least one electrodynamic ion funnel positioned in a reduced atmosphere environment; andat least one electrospray transmitter positioned in a direct relationship with said electrodynamic ion funnel whereby a preselected portion of a plume emitted by said electrospray transmitter is received within said electrodynamic ion funnel.

20. The system of claim 19, further comprising a second electrodynamic ion funnel.

21. The system of claim 19, wherein said electrospray transmitter is positioned within a reduced atmosphere environment.

22. The system of claim 21, wherein said electrodynamic ion funnel and said electrospray transmitter are located within the same reduced atmosphere environment.

23. The system of claim 19, wherein said electrospray transmitter is located at the receiving aperture of said first electrodynamic ion funnel.

24. The system of claim 19, wherein said electrospray transmitter is located within the receiving aperture of said first electrodynamic ion funnel.

25. The system of claim 19, wherein said electrospray transmitter is positioned a preselected distance from said first electrodynamic ion funnel, whereby the entire ion plume is captured within said first electrodynamic ion funnel.