Method and instrument for mass analyzing samples with a quistor

Abstract: A method for the measurement of mass spectra by three dimensional quadrupole fields (QUISTORs) is presented, in which the ions are mass-to-charge selectively ejected by the effect of a natural sum resonance in an inharmonic QUISTOR. In order to enhance scan speed and mass resolution, the ejection of a single kind of ions can be confined to a very small time interval, either by the generation of ions within a small volume outside the field center, or by an excitation of the secular amplitudes by an additional RF voltage across the end electrodes, shortly before the ions encounter the sum resonance condition in the course of the scan. An instrument for this method is described.

Description: The present invention presents a method and an instrument for the fast measurement of mass spectra from sample molecules, a so-called "scanning procedure", using a QUISTOR mass spectrometer. This special type of mass spectrometer, invented by Paul and Steinwedel (DE-C-944,9⊘⊘; filed 1954; U.S.-A-2 939 952), can store ions of different mass-to-charge ratios simultaneously in its radio-frequency hyperbolic three-dimensional quadrupole field. In the literature, it was later called "QUISTOR" ("QUadrupole Ion STORe") or "quadrupole ion trap" . (For a detailed introduction see Peter H. Dawson (editor), Quadrupole Mass Spectrometry And Its Applications, Elsevier, 1976). The QUISTOR usually consists of a toroidal ring electrode and two end cap electrodes. A high RF voltage with amplitude V stor and frequency f stor is applied between the ring electrode and the two end caps, possibly superimposed by a DC voltage. The hyperbolic RF field yields, integrated over a full RF cycle, a resulting force on the ions directed towards the center. This central field of force forms, integrated over time, an oscillator for the ions. The resulting oscillations are called the "secular" oscillations of the ions within the QUISTOR field. The secular movements are superimposed by the oscillation impregnated by the RF storage field. In general cylindrical coordinates are used to describe the QUISTOR. As indicated in figure 2 the direction from the center towards the saddle line of the ring electrode is called the r direction or r plane. The z direction is defined to be normal to the r plane, and located in the axis of the device. Up to now, the exact mathematical description, in an explicit and finite form, of the movements of ions in a QUISTOR field is only possible for the special case of independent secular movements in r and z direction. (For more details see Dawson 1976, and Paul and Steinwedel, 1956). The solution of the corresponding "Mathieu"'s differential equations results in a QUISTOR of fixed design with an angle of z/r = 1/1.414 (1.414 = square root of 2) of the double-cone which is asymptotic to the hyperbolic field. In this case, the central force is exactly proportional to the distance from the center, and exactly directed towards the center. This defines a harmonic oscillator, and the resulting secular movements are exactly harmonic oscillations. In this special case of an "harmonic QUISTOR", the secular oscillations can be calculated. The frequencies are usually plotted as "beta" lines in a so-called "a/q" diagram, where "a" is proportional to the DC voltage between ring and end electrodes, and "q" is proportional to the RF voltage. The beta lines describe exactly the secular frequencies in r and z direction: f sec,r = beta r * f stor / 2; f sec,z = beta z * f stor / 2. In figure 1, the "a/q" diagram with iso-beta lines is shown. In the "stability" area defined by ⊘ < beta r < 1 and ⊘ < beta z < 1, the secular oscillations of the ions are stable. Outside this stability area, the forces on the ions are directed away from the field center, and the oscillations are unstable. Up to now, two basically different modes of scanning procedures for stored ions of a wide range of mass-to-charge ratio by mass-to-charge selective ejection of ions have become known. First, US-A-4 54⊘ 884 (George C. Stafford, Paul E. Kelley, and David R. Stephens, filed 1982; EP-A-⊘ 113 2⊘7) describes a "mass selective instability scan". The quadrupole field is scanned in such a way that ions with subsequent mass-to-charge ratios encounter a destabilization by the conditions at or even outside the stability area border with beta z = 1. These ions become unstable, leave the quadrupole field, and are detected as they leave the field. Second, US-A-4 736 1⊘1 (John E.P. Syka, John N. Louris, Paul E. Kelley, George C. Stafford, Walter E. Reynolds, filed 1987; EP-A-⊘ 2⊘2 943) describes a scan method making use of the mass selective resonant ion ejection by an additional RF voltage across the end electrodes which is well-known from e.g. J. E. Fulford, D.-H. Hoa, R. J. Hughes, R. E. March, R. F. Bonner, and G. J. Wong, J. Vac. Sci. Technol., 17, (198⊘), 829: "Radio-frequency mass selected excitation and resonant ejection of ions in a three-dimensional quadrupole ion trap". In a pending EP-A-33 699⊘ (J. Franzen, R.H. Gabling, G. Heinen, and G. Weiß, filed 1988), we described an improvement of the second scan method by an enhancement of the resonant ion ejection using sum resonance effects in inharmonic QUISTORs. This invention is directed to a third basically different scanning procedure making primary use of the sharp natural resonance conditions in inharmonic QUISTORs. Most of the QUISTORs which have been built up to now, especially QUISTORs for high mass resolution scans, follow the design principles of "harmonic QUISTORs" with hyperbolic surfaces and the above "ideal" angle z/r = 1.414 , although it has been shown experimentally that QUISTORs of quite different design, e.g. with cylindrical surfaces, can store ions, even if these devices may encounter losses of specific ions. In "inharmonic QUISTORs" which are not built according to above ideal design criteria, the secular oscillations in one direction are coupled with the secular oscillations in the other direction. As it is known from coupled oscillators, natural resonance phenomena appear. Depending on the type of field distortions, several types of natural resonances, called "sum resonances" or "coupling resonances", exist in a QUISTOR. These natural resonances were experimentally investigated first by F. von Busch and W. Paul, Z. Phys. 164 (1961) 588, and explained theoretically by the effect of superimposed weak multipole fields. For more experimental work see Dawson 1976. These natural resonance phenomena were investigated intensively because they caused losses of ions from the QUISTOR, so workers in the field tried to avoid these resonances. See, e.g. P. H. Dawson and N. R. Whetten, J. Mass Spectrometry and Ion Physics, 2 (1969) 45: "Non-Linear Resonances in Quadrupole Mass Spectrometers due to Imperfect Fields. I. The Quadrupole Ion Trap". If the quadrupole field is superimposed by a weak multipole field, with one pole fixed in z direction, the conditions for sum resonances are: Type of field sum resonance condition Order of potential terms quadrupole field: none second order, no mixed terms hexapole field: beta z + beta r /2 = 1 third order, with mixed terms octopole field: beta z + beta r = 1 fourth order, with mixed terms dodecapole field: beta z /2 + beta r = 1 sixth order, with mixed terms In the case of a strictly harmonic QUISTOR with its exact quadrupole field, the mathematical expression for the electrical potential contains only quadratic terms in r and z, and no mixed terms. No sum resonance exists. In the case of superimposed multipoles, however, terms of higher order and mixed terms appear. The mixed terms represent the mutual influence of the secular movements, and the terms of higher order than 2 represent non-harmonic additions which make the secular frequencies dependent on the amplitude of the secular oscillations. (For the exact formulae of multipole potentials, see Dawson 1976). In the literature (see Dawson 1976), the superposition of small multipole fields are often designated as "distortions" or "imperfections". In case of inharmonic QUISTOR fields, the distortion of the field can be described as a finite or infinite sum of coaxial rotation-symmetric three-dimensional multipole fields. Such an inharmonic QUISTOR field can be generated by distortions of the ideal electrode geometry or by distortions of the applied RF voltage (e. g. by odd harmonics of the sine oscillation of thr RF voltage) or by a combination of both. The sum resonance conditions form distinct curves in the a/q stability diagram. (1, The conditions beta r + beta z /2 = 1 , beta r + beta z = 1 , and beta r /2 + beta z = 1 are plotted into the diagram given in fig. 1). If an ion fulfils the sum resonance condition, its secular frequency movement amplitude increases, and the ion leaves the field if the condition for resonance lasts. A first embodiment of the invention is obtained by the features of the claims 1 and 21. This invention is based on our observations (1) that it is possible to create field configurations which support essentially a single sum resonance condition only, and (2) that sum resonances can be made to have extremely narrow bandwidths (they are extremely sharp). For a good mass spectrometric resolution between ions of different mass-to-charge ratios, all ions of the same mass-to-charge ratio have to be ejected almost simultaneously. Encountering a sum resonance condition, ions with small secular amplitudes increase their amplitudes slower than ions with large amplitudes. To eject ions of the same kind within a very small time interval, it is, therefore, necessary to force ions of the same kind to have almost equal secular amplitudes. The invention, therefore, provides an additional method of producing the ions in a small volume located outside the center of the storage field. If ions are produced in such a way, they show very similar secular movement amplitudes. This method requires a good vacuum within the QUISTOR so that the ion secular movements are not damped by collisions with residual gas molecules. The invention provides a second additional method to enhance the resolution during ion ejection: Ions are either generated in the field center (for a method see DE-A-37 ⊘⊘ 337.2; J. Franzen, and D. Koch; filed 1987), or damped by a gas added to cause the ion secular movements collapse into the center by repeated collisions. The secular oscillations of the ions to be ejected are then increased selectively by resonance with an additional RF field across the center, a short time before they encounter the sum resonance by the scanning RF quadrupole storage field. If the frequency of the additional RF is chosen a little lower then the frequency of the sum resonance condition, and the storage field is scanned towards higher storage RF voltages, the ions of a selected mass-to-charge ratio first start to resonate within the additional RF field. They increase thereby their secular movement amplitudes synchronously. In the progress of the scan, and eventually before the ion movements are damped again by the damping gas, the ions encounter the sum resonance condition, and leave the QUISTOR field synchronously. If the frequency of the additional RF field is tuned into the frequency of the sum resonance condition, a double resonance effect appears, as described in our EP-A-33 69⊘. The effect on the resolution is similar, but the exact tuning of the additional RF frequency into the sum resonance frequency makes this method by far more difficult. The present method, furthermore, has the advantage, that small shifts of the sum resonance frequency, caused e.g. by surface charges on the QUISTOR electrodes, do not disturb the operation. A hitherto best inharmonic QUISTOR mass spectrometer (fig. 2) can be designed by ring (4) and end electrodes (3), (5), formed precisely hyperbolically with an angle 1:1.385 of the hyperbole asymptotes. The electrodes are spaced by insulators (7) and (8). Ions may be formed by an electron beam which is generated by a heated filament (1) and a lens plate (2) which focuses the electrons through a hole (1⊘) in the end cap (3) into the inharmonic QUISTOR during the ionization phase, and stops the electron beam during other time phases. The movement of the ions inside the inharmonic QUISTOR is damped by the introduction of a damping gas of low molecular weight through entrance tube (11). Among other damping gases, like Helium, normal air at a pressure of 3 * 1⊘⁻² Pa (3 * 1⊘⁻⁴ mbar) turns out to be very effective. The sum resonance frequency f res,z in z direction, in this case obeying the resonance condition f res,z + f res,r = f stor /2, can be measured to be about f res,z = ⊘.342 * f stor . Using a storage frequency of f stor = 1 MHz, the additional frequency across the end electrodes can be chosen as f exc = 333.333 kHz. The latter can be advantageously generated from the oscillator which produces the frequency of the storage voltage, by a frequency division. The optimum voltage of the exciting frequency depends a little on the scan speed, and ranges from 1 Volt to about 2⊘ Volts. During the scan period, ions are ejected through the perforations (9) in the end cap (5), and measured by the multiplier (6). With an inner radius of the ring electrode (4) of r o = 1 cm, and with ions stored in the QUISTOR during a preceding ionization phase, a scan of the high frequency storing voltage V stor from a storage voltage upwards to 7.5 kV yields a spectrum up to more than 5⊘⊘ atomic mass units in a single scan (Fig. 3). A full scan over 5⊘⊘ atomic mass units can be performed in only 1⊘ milliseconds. This is the fastest scan rate which has been reported for a QUISTOR. The basic idea of this invention is the mass selective ejection of charged particles, caused by sum-resonances occuring in path-stability spectrometers due to imperfect fields. It is therefore to be understood that, within the scope of the present claims, the invention may be practiced otherwise than specifically described. Figure captures Fig. 1: Stability area for an "ideal" QUISTOR in the a z / q z diagram, with iso-beta lines. Resonance condition lines for hexapole, octopole, and dodekapole field faults are given, crossing the iso-beta lines. Fig. 2: Design of an inharmonic QUISTOR mass spectrometer. The angle of the asymptote measures 1:1.385. Other details are given in the text. Fig. 3: Portion of a mass spectrum measured by a scan of the 1 MHz storage RF voltage amplitude with an inharmonic QUISTOR. Shown here is a single scan measurement of trimethyl benzene. The full spectrum covered the mass range from 4⊘ amu to 5⊘⊘ amu, and was measured in 9.2 milliseconds. With 1 millisecond ionization time, and 8 milliseconds of damping in 4 * 1⊘⁻² Pa (4 * 1⊘⁻⁴ mbar air), the total spectrum generation took less than 2⊘ milliseconds. The secular amplitudes of the ions were increased by resonance with a 333,333 kHz additional voltage of 3 Volts only across the end electrodes, prior to an exposition of the ions to the sum resonance condition.

Claims: A method of measuring by means of a Quistor a mass spectrum of sample material which comprises the steps of defining a three-dimensional electrical ion storage field in which ions with mass-to-charge ratios in a range of interest can be simultaneously trapped; introducing or creating sample ions into the quadrupole field whereby ions of interest are simultaneously trapped and perform mass-to-charge specific secular movements; changing the quadrupole field so that simultaneously and stably trapped ions of consecutive mass-to-charge ratios encounter a sum resonance of their secular movements, increase thereby their secular movement amplitudes, and leave the trapping field; and detecting the ions of sequential mass-to-charge ratios as they leave the trapping field, characterized in that the ion storage field consists of an inharmonic quadrupole field. The method of claim 1 in which the inharmonic quadrupole ion storage field is generated by distortions of the ideal electrode geometry or by distortions of the wave form of the applied RF voltage or by a combination of both. The method of claim 1 or 2 in which the inharmonic quadrupole ion storage field is generated by the superposition of an exact quadrupole field with a finite or infinite sum of co-axial multipole fields. The method of claim 1, 2 or 3 in which the storage field is generated by a QUISTOR of the type having a ring electrode and spaced end electrodes where the inharmonic quadrupole field is generated by additional electrodes between the ring and end electrodes. The method of claim 1, 2 or 3 in which the storage field is generated by a QUISTOR of the type having a ring electrode and spaced end electrodes where the inharmonic quadrupole field is generated by the shape of the electrode surfaces. The method of claim 5 in which the QUISTOR has the shape of two rotation-symmetric hyperbolic end caps and a rotation-symmetric hyperbolic toroid with an angle of the inscribed asymptotic double-cone deviating from 1:1.414. The method of claim 6 with a cone angle between 1:1.34 and 1:1.410. The method according to one of the claims 1 to 7, characterized in that the ions stored in the field are generated outside the exact center of the field. The method of claim 8 in which the ions are generated in a distinct location outside the center of the field. The method of claim 9 in which the ion generation is located in the r-plane in a distance from the field center of about 1/8 to 1/6 of the inner diameter of the ring electrode. The method of claim 9 in which the ion generation is located in the field axis in a distance of about 1/8 to 1/4 of the distance between the end electrodes. The method of one of the foregoing claims in which the inharmonic quadrupole field supports the sum resonance condition beta r + beta z = 1 . The method according to one of the claims 1 - 12, characterized in that the ions stored in the center of the storage field are modulated by an additional RF field, whereby the frequency of the additional RF field differs from the axial secular movement frequency of the ions encountering the sum resonance. The method according to one of the claims 4 to 12 in which the additional RF field for ion modulation (introduced in claim 13) is generated by an additional RF voltage between the end electrodes. The method of claim 13 or 14 in which the ions encounter a resonance with the additional RF field just before they encounter the sum resonance condition during the change of the RF storage field. The method of one of the claims 13 to 15 in which the additional RF field frequency equals exactly 1/n of the RF storage field frequency, n being an integer number > 2. The method of claim 16 in which the additional RF field frequency is phase-locked to the RF storage field frequency. The method of one of the claims 13 to 17 in which the ions are generated in the field center. The method of one of the claims 13 to 17 in which the secular ion movements in the storage field are damped by a damping gas. The method as of one of the foregoing claims characterized in that the drift of the frequency of the sum resonance which is caused by the change of the storage field, equals the drift of the frequency of the resonating ions which is caused by the growth of their secular movement amplitudes in the inharmonic quadrupole ion storage field. A mass spectrometer comprising a QUISTOR with means to generate an ion storage field, means for introducing or generating ions within the storage field, means for detecting ions leaving the storage field, and means to vary the storage field to cause ions of subsequent mass-to-charge ratios exit the field sequentially merely by an increase of their secular amplitudes induced by sum resonances of their secular movements, characterized in that the ion storage field consists of an inharmonic quadrupole field. The mass spectrometer as of claim 21 with the inharmonic quadrupole field generated by an ideal quadrupole field superimposed by a sum of coaxial multipole fields. The mass spectrometer as of claim 22 characterized in that the inharmonic quadrupole storage field is produced by a ring electrode and two end electrodes shaped to yield the basic quadrupole and superimposed coaxial multipole fields. The mass spectrometer as of claim 23 with rotation-symmetrical hyperbolic electrodes with an angle of the asymptotic cone deviating from 1:1.414. The mass spectrometer as of claim 24 with an angle between 1:1,34 and 1:1,40.

Inventors: FRANZEN JOCHEN DR, GABLING REEMT-HOLGER DR, HEINEN GERHARD, WEISS GERHARD, FRANZEN, JOCHEN, DR., GABLING, REEMT-HOLGER, DR., HEINEN, GERHARD, WEISS, GERHARD
Applicants: BRUKER FRANZEN ANALYTIK GMBH
Application year: 1989
Main classification: H01J49
IPC codes: H01J49