Radiant energy – Ionic separation or analysis – Ion beam pulsing means with detector synchronizing means
Reexamination Certificate
2002-02-21
2004-11-09
Lee, John R. (Department: 2881)
Radiant energy
Ionic separation or analysis
Ion beam pulsing means with detector synchronizing means
C250S287000
Reexamination Certificate
active
06815669
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to chemical analytical systems based on ion mobility, and conveyance of ions through such a system.
BACKGROUND OF THE INVENTION
The ability to detect and identify explosives, drugs, chemical and biological agents as well as monitor air quality has become increasingly more critical given increasing terrorist and military activities and environmental concerns. Previous detection of such agents was accomplished with conventional mass spectrometers, time of flight ion mobility spectrometers and conventional field asymmetric ion mobility spectrometers (FAIMS).
Mass spectrometers are very sensitive and selective with fast response time. Mass spectrometers, however, are large and require significant amounts of power to operate. They also require a powerful vacuum pump to maintain a high vacuum in order to reduce ion neutral interactions and permit detection of the selected ions. Mass spectrometers are also very expensive.
Another spectrometric technique which is less complex is time of flight ion mobility spectrometry which is the method currently implemented in most portable chemical weapons and explosives detectors. The detection is based not solely on mass, but on charge and cross-section of the molecule as well. However, because of these different characteristics, molecular species identification is not as conclusive and accurate as the mass spectrometer. Time of flight ion mobility spectrometers typically have unacceptable resolution and sensitivity limitations when attempting to reduce their size. In time of flight ion mobility, the resolution is proportional to the length of the drift tube. The longer the tube the better the resolution, provided the drift tube is also wide enough to prevent all ions from being lost to the side walls due to diffusion. Thus, fundarnentally, miniaturization of time of flight ion mobility systems leads to a degradation in system performance. While conventional time of flight devices are relatively inexpensive and reliable, they suffer from several limitations. First, the sample volume through the detector is small, so to increase spectrometer sensitivity either the detector electronics must have extremely high sensitivity, requiring expensive electronics, or a concentrator is required, adding to system complexity. In addition, a gate and gating electronics are usually needed to control the injection of ions into the drift tube.
FAIMS spectrometry was developed in the former Soviet Union in the 1980's. FAIMS spectrometry allows a selected ion to pass through a filter while blocking the passage of undesirable ions. But the only commercial prior art FAIMS spectrometer was large and expensive, e.g., the entire device was nearly a cubic foot in size and cost over $25,000. Such systems are not suitable for use in applications requiring small detectors. They are also relatively slow, taking as much as one minute to produce a complete spectrum of the sample gas, are difficult to manufacture and are not mass producible.
The prior art FAIMS devices depend upon a carrier gas that flows in the same direction as the ion travel through the filter. However, the pumps required to draw the sample medium into the spectrometer and to provide a carrier gas can be rather large and can consume large amounts of power.
It is therefore an object of the present invention to provide an ion filter and detection system which does not require the high flow rate, high power consumption pumps normally associated with FAIMS spectrometers.
It is another object of the present invention to provide method and apparatus for highly efficient conveyance of ions into and through a high field ion mobility filter.
It is a further object of the present invention to provide method and apparatus for efficient conveyance of ions into and through a high field ion mobility filter without the use of a carrier gas.
It is another object of the present invention to provide a FAIMS filter and detection system which can quickly and accurately control the flow of selected ions to produce a sample spectrum.
It is a further object of the present invention to provide a FAIMS filter and detection system which has a sensitivity of parts per billion to parts per trillion.
It is a further object of the present invention to provide a FAIMS filter and detection system which may be packaged in a single chip.
It is a further object of the present invention to provide a FAIMS filter and detection system which is cost effective to implement, produce and operate.
SUMMARY OF THE INVENTION
The present invention features an ion mobility spectrometer for filtering ions via an asymmetric electric field. Ions are transported along the longitudinal ion flow path via an ion flow generator. The ion flow generator preferably provides ion propulsion via a local electric field in the flow path. Operation of the invention enables elimination or reduction of flow rate and power requirements of conventional gas flow.
In a preferred embodiment, a longitudinal electric field generated by the ion flow generator propels ionized sample received from an ionization region through a compensated, asymmetric electric field of the ion filter, with a desired species passing through the filter and flowing toward a detector region. Various options are possible. In one embodiment, a low volume gas flow carries the sample to the filter. In other embodiment, there is no need for gas flow and ion steering, or the longitudinal field itself, propels ions into the filter region, where the ions are further propelled by the ion flow generator.
In another embodiment, a supply of clean filtered air is flowed in the negative longitudinal direction opposite the desired direction of ion flow to keep the ion filter and detector regions free of neutrals and to help remove solvent, reduce clustering, and minimize the effects of humidity.
A preferred embodiment of the present invention features an ion mobility spectrometer having a housing structure that defines a flow path (also known as a drift tube) that begins at a sample inlet for receipt of sample (i.e., sample molecules to be analyzed) and brings the sample to an ionization region. Once ionized, the sample passes to the ion filter, with desired ion species passing through the filter in the flow path, as propelled by the ion flow generator.
In one embodiment, the ion filter is provided with a plurality of high frequency, high voltage filter electrodes for creation of the asymmetric electric field transverse to the longitudinal ion flow direction along the flow path. In a preferred embodiment, this field is compensated, to pass only a desired ion species for downstream detection. In another embodiment, filtering is trajectory based without requiring compensation.
The ion flow generator creates a longitudinal electric field along the flow path (transverse to the asymmetric electric field) for propelling or transporting the ions through the asymmetric electric field toward the output region to enable detection and analysis. The ionization source may include a radiation source, an ultraviolet lamp, a corona discharge device, electrospray nozzle, plasma source, or the like.
In one embodiment, an electric controller supplies a compensation bias and an asymmetric periodic voltage to the ion filter. The ion filter typically includes a pair of spaced electrodes for creating the asymmetric electric field between the electrodes. The ion flow generator typically includes a plurality of spaced discrete electrodes proximate to the filter electrodes for creating a longitudinal direction electric field which propels the ions through the transverse asymmetric electric field, and onward for detection. The ion filter and flow generator may share none, some or all electrodes.
In another embodiment, the ion flow generator includes spaced resistive layers and a voltage is applied along each layer to create the longitudinally directed electric field which propels the ions through the filter's compensated asymmetric electric field and to the detector.
In another embo
Miller Raanan A.
Zahn Markus
Gurzo Paul M.
Lee John R.
Ropes & Gray LLP
The Charles Stark Draper Laboratory Inc.
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