Abstract
The present invention relates to the technical field of mass analysis instruments. Disclosed is an ion excitation method in a linear ion trap. The method comprises: in a linear ion trap, and at an ion collision-induced dissociation stage, simultaneously applying an auxiliary excitation signal in radial X and Y directions thereof; increasing the kinetic energy of ions in the two directions, thereby increasing collisions with a center gas to cause dissociation; and converting the kinetic energy to internal energy to achieve tandem mass spectrometry analysis. The kinetic energy in the X and Y directions of the ion is increased, and compared to a conventional dissociation method in which ions are primarily excited in one direction, more kinetic energy is converted to internal energy, thus improving dissociation efficiency, shortening reaction time, and addressing a low mass cutoff effect in the ion trap.
Claims
1. A method of ion excitation for dissociation in linear ion traps, comprising: Applying two dipolar or monopole AC excitation signals to x and y pairs of electrodes in linear ion traps to cause ions to undergo excitation simultaneously in the radial x and y directions
2. The method of claim 1, wherein the excitation AC signal only contain a single frequency.
3. The method of claim 1, wherein the excitation AC signal is the sum of multiple frequency components.
4. The method of claim 1, wherein the waveforms applying to the x electrodes and y electrodes can be the same type. In this case, the frequency, amplitude, phase difference of the two AC signals can be the same or different. the phase difference varies from 0 to 360 degrees, but does not include 90 degrees.
5. The method of claim 1, wherein the types of the two AC waveforms applying to the two pairs of electrodes are completely different.
6. The method of claim 1, wherein the mass spectrometer can be quadrupoles, linear ion trap with the hyperbolic electrodes, rectilinear ion trap, or a triangular-electrode linear ion trap.
7. The method of claim 2, wherein the waveforms applying to the x electrodes and y electrodes can be the same type. In this case, the frequency, amplitude, phase difference of the two AC signals can be the same or different. the phase difference varies from 0 to 360 degrees, but does not include 90 degrees.
8. The method of claim 3, wherein the waveforms applying to the x electrodes and y electrodes can be the same type. In this case, the frequency, amplitude, phase difference of the two AC signals can be the same or different. the phase difference varies from 0 to 360 degrees, but does not include 90 degrees.
9. The method of claim 2, wherein the types of the two AC waveforms applying to the two pairs of electrodes are completely different.
10. The method of claim 3, wherein the types of the two AC waveforms applying to the two pairs of electrodes are completely different.
11. The method of claim 2, wherein the mass spectrometer can be quadrupoles, linear ion trap with the hyperbolic electrodes, rectilinear ion trap, or a triangular-electrode linear ion trap.
Description
BRIEF DESCRIPTION OF THE FIGURES
[0024] FIG. 1 is using a quadrupole as a model of a linear ion trap, the present invention employs an auxiliary voltage signal application diagram implemented in a dipole manner.
[0025] FIG. 2 is a schematic illustration of an implementation circuit of a specific embodiment 1 of the present invention, wherein a triangular electrode ion trap is used as a linear ion trap.
[0026] FIG. 3a: embodiment 1, is a simulation of the ion motion trajectory of 10 mass-to-charge ratio 556 ions in a conventional one-way excitation within 20 ms.
[0027] FIG. 3b; embodiment 1, simulation of the ion motion trajectory of 10 mass-to-charge ratio 556 ions in the inventive two-way excitation within 20 ms.
[0028] FIG. 4a: embodiment 1, simulation of the ion x-direction motion trajectory for mass-to-charge ratio 556 ions in the traditional one-way excitation as a function of time
[0029] FIG. 4b: embodiment 1, simulation of the ion y-direction motion trajectory for mass-to-charge ratio 556 ions of the present invention under the two-way excitation as a function of time.
[0030] FIG. 5a: embodiment 1, simulation of ion radial kinetic energy Er for mass-to-charge ratio 556 ions in the traditional one-way excitation as a function of time.
[0031] FIG. 5b: embodiment 1, simulation of ion radial kinetic energy Er for mass-to-charge ratio 556 ions of the present invention under the two-way excitation over time
[0032] FIG. 6: a schematic diagram of the structure of the instrument platform of embodiment 1.
[0033] FIG. 7a: embodiment 1, the ratio of the fragment ion a4/b4 of the enkephalin sample to the q value in the conventional one-way excitation (represented by 1) and the two-way excitation of the present invention (represented by 2)
[0034] FIG. 7b: embodiment 1, the relationship between the fragmentation efficiency and the value of q for an enkephalin sample in both conventional one-way excitation and two-way excitation of the present invention
[0035] FIG. 8a: embodiment 1, a tandem mass spectrum under one-way excitation of the enkephalin sample of embodiment 1 with an excitation amplitude of 200 mV and an excitation time of 20 ms, obtaining the same energy deposition (fragment ion a4/b4=3).
[0036] FIG. 8b: embodiment 1, a tandem mass spectrum under two-way excitation of the enkephalin sample of embodiment 1 with an excitation amplitude of 200 mV and an excitation time of 20 ms, obtaining the same energy deposition (fragment ion a4/b4=3).
DETAILED DESCRIPTION
[0037] The present invention will now be described in further detail with reference to the accompanying embodiments and drawings.
[0038] In the present invention, ions in the linear quadrupole devices are excited in the two-ways by applying auxiliary excitation signals in the x and y directions. Compared to the conventional single-way excitation method, the ion kinetic energy is increased and therefore more internal energy will be deposited into ions during collision-induced dissociation. FIG. 1 is an embodiment of the present invention wherein two auxiliary excitation signals are applied in dipolar fashion to the two pairs of electrodes in one embodiment of the invention. As the quadrupole is a model of a linear ion trap, the invention is applicable to all linear ion traps. Two RF signals with opposite phases are fused by a condensed line to an auxiliary AC signal and then were applied to a pair of opposing electrodes. The RF Signals are identical to the AC signal but 180 degrees out of phase. That is to say, AC signal is applied in dipolar fashion. AC signal can also be applied to only one electrode of each pair and this is in monopolar fashion. The auxiliary AC signal can be various types of waveforms which contain only one frequency component, such as sinusoidal wave, triangular wave, and square wave signals. It can also be waveforms which is the superimposition of several or a number of frequency components, such as noise signal, stored waveform inverse Fourier Transform (SWIFT) signal and so on. The two auxiliary excitation signals AC1 and AC2 can be the same type, for example both are sinusoidal wave. They can also be different types of AC signals, for example, AC1 is sine wave, and AC2 is square wave. If the two AC signals are the same type, the AC1 and AC2 can be exactly the same, including the amplitude, frequency, and phase. If it is a square wave signal of a single frequency, the duty ratios of the two signals may be the same or different.
[0039] Embodiment 1, FIG. 2 which shows a schematic illustration of the electric circuit for the superposition of dipolar AC in a dipole manner in triangular-electrode linear ion trap. An auxiliary AC waveform produced by the control system is separated into two equal AC signals, as depicted in FIG. 2. One AC signal is coupled to one RF signal through a switch and then applied to the electrodes. The other AC signal was also coupled to the out-of-phase RF signal and then applied to the other electrodes. The signal switch can control whether the auxiliary AC signal is put out and not put out in different timing stages CID experiments involve several stages including ion injection, ion cooling, ion isolation, collision-induced dissociation, and mass analysis. For conventional CID, the switch is off at all time and there is no auxiliary AC signal output.
[0040] FIGS. 3, 4 and 5 show the simulation results of ion trajectory and ion kinetic energy according to the first embodiment of the present invention. The specific simulation conditions are q=0.25 for the ion-to-charge ratio of 556, the excitation signal amplitude is 100 mV, the collision gas is nitrogen, the gas pressure is 008 mTorr, and the temperature is 300 Ka. FIG. 3 illustrates that ions can be resonantly excited in x- and y-directions simultaneously by applying two dipolar AC signals to the two pairs of LIT electrodes. The excitation signal frequency is adjusted to the optimal value, that is, the ion kinetic energy is the largest, the other conditions are exactly the same, and the displacement of the ions in the X and Y directions is shifted. It can be seen that the solution of the invention allows ions to be simultaneously excited in both directions. FIG. 4 further shows a simulation of the trajectory of ions in the xy plane. For excitation in both directions, ions move approximately along the line x=y, and, for conventional excitation in one direction, along the line y=0. FIG. 5 shows the relationship between the unidirectional particle kinetic energy of a particle with time, the maximum kinetic energy of the two-way excitation is 32 eV, and the unidirectional is 25 eV, the method increases the ion kinetic energy by nearly 30%.
[0041] FIGS. 6-8 show the results of verification of the experimental protocol in embodiment 1 FIG. 6 shows experimental set-up for the electrospray ion source-delta electrode ion trap mass spectrometer designed and used by the laboratory itself. It is a homemade three-stage differential pumping vacuum system. The vacuum chamber in the vacuum chamber can reach a vacuum of 105 Torr. The nitrogen gas is used as the cooling gas. The gas pressure is maintained at 8105. The ions generated by the Torra electrospray ion source pass through the sampling plate. The sampling cone enters the second-stage vacuum chamber and enters the triangular electrode ion trap mass analyzer under the transmission of a 200 mm long quadrupole ion guiding rod. Reagent: Leucine encephalin (m/z 556, Gil Biochemical Shanghai Co., Ltd.), solvent:methanol:water=50:50, which contains 0.5% acetic acid. The brain endorphin sample is a standard sample for studying the ion dissociation of electrospray ionization mass spectrometry. The ratio of the fragment ions a4 and b4 can reflect the internal energy of the ion deposition. The larger the ratio, the larger the internal energy of the deposition.
[0042] The experimental conditions in FIGS. 7 and 8 are as follows: the dissociation time is 20 ms, the excitation signal amplitude is 200 mV, and the excitation frequency is optimized to maximize the fragmentation efficiency or the ratio of a4 to b4. FIG. 7a reflects that the parent ion brain endorphin q is in the range of 0.23 to 0.42. The ion two-way excitation of the present invention is higher than the conventional one-way excitation of a4 and b4, that is, the internal energy of deposition is more, and the larger q is, the more obvious the effect. FIG. 7b is reflects a lower q value, and the two-way excitation fragmentation efficiency of the present invention is higher. FIG. 8 shows mass spectra of the CID results of protonated leucine enkephalin when a4/b4=3. FIG. 8a is the mass spectrum of the conventional one-way excitation, q is 0.33. FIG. 8b is
[0043] the mass spectrum of the two-way excitation of the present invention, q is 0.43. It can be seen that this method can observe more fragment ions.
