Patent Application
20080067355
An example of a mass spectrometer interface is an electrospray ionization (ESI) system. In such a system, a source uses a capillary to deliver a sample solution from a sample pump, or from a liquid or gas chromatographic effluent, to an ionizer, such as a metal or metalized needle, at a location near the mass spectrometer interface. By applying an electric field between the needle and the interface, charged droplets are generated as a continuous spray.
In a prior art embodiment (
While charged droplets 12 enter the first orifice 8, a heated drying gas stream (usually nitrogen gas) is sent across the space between two plates 2 and 4. By colliding with drying gas molecules, the charged droplets 12 undergo a desolvation process and become single or multiple charged ions. These ions continue to propagate into vacuum via the second orifice 10, and are analyzed by a mass spectrometer (not shown).
During the time crossing between the first and second orifices 8 and 10, many of the droplets 12 are carried away by drying gas, and become waste. Some of the droplets 12 survive the desolvation and enter the vacuum chamber of the mass spectrometer. This portion of incompletely desolvated droplets 12 contributes largely to the signal noise and sacrifices instrument sensitivity.
Embodiments of the invention include a mass spectrometer sample input interface comprising a desolvation apparatus and an ion pathway apparatus. The desolvation apparatus defines a desolvation pathway along which a desolvation gas flows, in a direction from upstream to downstream. The ion pathway apparatus defines an ion pathway for analyte solution droplets to follow, the ion pathway leading into the mass spectrometer. The desolvation pathway has a desolvation pathway portion; and the ion pathway includes an ion pathway portion that follows the desolvation pathway portion.
The desolvation apparatus includes a structure, made up of one or more members, for directing the desolvation gas along the desolvation pathway. For instance, the desolvation apparatus may include first and second desolvation pathway members, disposed so as to define the desolvation pathway therebetween.
The structure includes a sample entrance and a sample exit, and a portion of the ion pathway runs between them. For instance, the sample entrance and the sample exit may be disposed at different points within the desolvation apparatus, such as within the first and second desolvation pathway members, respectively. The sample exit is downstream from the sample entrance.
The embodiment additionally includes an ion pathway apparatus. In
The ion pathway apparatus defines an ion pathway, in which sample droplets 12 that are ionized by an ionizer apparatus, for instance including an ion source 14, travel through the first orifice 8 and the second orifice 10, along an ion pathway portion therebetween. The ion pathway portion leads from the first orifice 8, along the desolvation pathway portion, to the second orifice 10. Because the desolvation pathway portion runs from upstream to downstream, as does the desolvation pathway as a whole, likewise the ion pathway portion runs upstream to downstream.
The ion source 14 can be implemented according to various types of electrospray ionization. For instance it can include gas assisted spray, gas-free spray, micromachined spray tips, and/or spray tips made on a chip. For purposes of the present patent application, the terms “spray needle” and “spray tip” will be used interchangeably, and their meaning is in accordance with known terminology as outlined here.
Alternatively, other atmospheric pressure ionization sources such as atmospheric pressure chemical ionization (APCI), atmospheric pressure photo ionization (APPI), and atmospheric pressure matrix assisted laser desorption/ionization (AP-MALDI) may be used.
As shown in
As the charged droplets 12 enter the first orifice 8, they continue to propagate towards the second plate 4. For instance, an electrical potential difference may be applied to the plates 2 and 4, generating an electrical field which attracts the charged droplets 12 and ions toward the second orifice 10. The potential difference may be user-adjustable for optimum performance.
However, because of the axial offset 16, the sample droplets 12 travel along an ion pathway portion, which coincides with and follows the desolvation pathway portion. Because of this ion pathway portion, the droplets 12 travel a greater distance, within the desolvation gas stream, than would be the case if the orifices 8 and 10 were directly aligned with each other and the ion pathway merely crossed perpendicular to the desolvation pathway.
By traveling this additional distance, the droplets 12 have a greater amount of time, and exposure to desolvation gas, to more completely undergo the desolvation process. More ions are generated, and fewer droplets remain, and enter the mass spectrometer for analysis. As a result, the mass spectrometer's analyte signal is enhanced.
It remains true, of course, that a portion of the droplets 12 are carried away by the gas flow, before they pass through the second orifice 10. However, sufficient ions remain for the mass spectrometer effectively to perform its analysis.
Since the two orifices 8 and 10 are offset, there is no direct line-of-sight in the path of the droplets 12. Because of this, incompletely desolvated droplets 12 are less likely to enter the second orifice 10. Thus, the mass spectrometer analysis is less affected by errors (sometimes characterized as “noise”) caused by such droplets 12. As a result, the signal-to-noise ratio, and hence the mass spectrometer sensitivity, is increased.
The embodiment of
In one embodiment of the invention, one or both of the plates 2 and 4 are adjustable in the direction of the drying gas flow, i.e., the axial offset of two orifices 8 and 10 is adjustable. The adjustment provides the possibility for optimizing the duration of desolvation time for different samples and flow rates. In another embodiment, he distance between the plates 2 and 4 is also variable so the signal-to-noise ratio can further be optimized.
In yet another embodiment, the orifices 8 and 10 may vary in size and shape, and the size and shape may be different, between the orifices 8 and 10. For instance, the first orifice 8 in the plate 2 on the atmospheric side may be larger than the second orifice 10 in the plate 4, facing the vacuum side.
In connection with the various embodiments just discussed, here are some dimensions for the various structures, which have been found to yield embodiments of the disclosed structure, that have worked well.
A gap between the first and second plates 2 and 4 can be 5 to 15 millimeters (mm), or more specifically about 10 mm. Where the first orifice 8 is circular in shape, its diameter can be 1 to 10 mm, or more specifically 3 to 6 mm. Likewise, where the second orifice 10 is circular, its diameter can be 1 to 5 mm, or more specifically 2 to 3 mm. Where the orifices 8 and 10 are both circular in shape, an offset distance between the orifices may conveniently be measured as an offset between their central axes. Such offset can be 1 to 10 mm, or more specifically 3 to 6 mm.
In another embodiment, the orifices 8 and 10 may be covered with porous voltage controllable members, such as conductive mesh grids. A selectable voltage, applied from a voltage source to one or both of such porous electrostatic members, will urge the ions through the orifices 8 and 10.
In a typical prior art embodiment in which the ion source 14 includes an elongated structure such as a spray needle, the spray needle is arranged parallel to the orifice plate, i.e., perpendicular to the orifice axis. This arrangement is widely used in a conventional spray interface to reduce noise by incompletely desolvated droplets entering the mass spectrometer. However, the need for such parallel configuration was a constraint brought about because of the line-of-sight alignment of the two orifices. This is because, in such conventional structures, the droplets 12 had an initial velocity which facilitated the passage of non-desolvated droplets 12 through the line-of-sight orifices into the mass spectrometer, with the resultant undesirable noise generation discussed above.
Embodiments of the invention can include an alignment apparatus (not shown) to align a position and/or an angular alignment of an ion source of an ionizer apparatus, relative to the ion pathway. The alignment apparatus may, in some embodiments, permit user adjustment of the ion source alignment.
In the embodiment of
In one alternative embodiment (
In another alternative embodiment (
Generally, the sensitivity of an atmospheric pressure ionization mass spectrometer is increased, when an interface structure embodying the invention is used. It has been found that mass spectrometers with sample input interfaces embodying the invention do not raise the manufacturing cost above that of mass spectrometers including prior art sample input interfaces. Moreover, since there is more flexibility for orienting spray tips relative to the interface, ionization of the sample droplets can be further optimized.
Although the present invention has been described in detail with reference to particular embodiments, persons possessing ordinary skill in the art to which this invention pertains will appreciate that various modifications and enhancements may be made without departing from the spirit and scope of the claims that follow.
