A new ion soft landing instrument has been built for the controlled deposition of mass selected polyatomic ions. The instrument has been operated with an electrospray ionization source; its major components are an electrodynamic ion funnel to reduce ion loss, a 90-degree bent square quadrupole that prevents deposition of fast neutral molecules onto the landing surface, and a novel rectilinear ion trap (RIT) mass analyzer. The ion trap is elongated (inner dimensions: 8 mm x 10 mm x 10 cm). Three methods of mass analysis have been implemented. (i) A conventional mass-selective instability scan with radial resonance ejection can provide a complete mass spectrum. (ii) The RIT can also be operated as a continuous rf/dc mass filter for isolation and subsequent soft landing of ions of the desired m/ z value. (iii) The 90-degree bent square quadrupole can also be used as a continuous rf/dc mass filter. The mass resolution (50% definition) of the RIT in the trapping mode (radial ion ejection) is approximately 550. Ions from various test mixtures have been mass selected and collected on fluorinated self-assembled monolayers on gold substrates, as verified by analysis of the surface rinses. Desorption electrospray ionization (DESI) has been used to confirm intact deposition of [Val (5)]-Angiotensin I on a surface. Nonmass selective currents up to 1.1 nA and mass-selected currents of up to 500 pA have been collected at the landing surface using continuous rf/dc filtering with the RIT. A quantitative analysis of rinsed surfaces showed that the overall solution-to-solution soft landing yields are between 0.2 and 0.4%. Similar experiments were performed with rf/dc isolation of both arginine and lysine from a mixture using the bent square quadrupole in the rf/dc mode. The unconventional continuous mass selection methods maximize soft landing yields, while still allowing the simple acquisition of full mass spectra.
Mass-selected polyatomic cations and anions, produced by electrosonic spray ionization (ESSI), were deposited onto polycrystalline Au or fluorinated self-assembled monolayer (FSAM) surfaces by soft landing (SL), using a rectilinear ion trap (RIT) mass spectrometer. Protonated and deprotonated molecules, as well as intact cations and anions generated from such molecules as peptides, inorganic catalysts, and fluorescent dyes, were soft-landed onto the surfaces. Analysis of the modified surfaces was performed in situ by Cs ϩ secondary ion mass spectrometry (SIMS) using the same RIT mass analyzer to characterize the sputtered ions as that used to mass select the primary ions for SL. Soft-landing times as short as 30 s provided surfaces that yielded good quality SIMS spectra. Chemical reactions of the surfaces modified by SL were generated in an attached reaction chamber into which the surface was transferred under vacuum. For example, a surface on which protonated triethanolamine had been soft landed was silylated using vapor-phase chlorotrimethylsilane before being returned still under vacuum to the preparation chamber where SIMS analysis revealed the silyloxy functionalization. SL and vapor-phase reactions are complementary methods of surface modification and in situ surface analysis by SIMS is a simple way to characterize the products produced by either technique. (J Am Soc Mass Spectrom 2009, 20, 949 -956)
A multichannel mass spectrometer based on the rectilinear ion trap (RIT) analyzer was designed and constructed for simultaneous high-throughput analysis of multiple samples. The instrument features four parallel ion source/mass analyzer/detector channels assembled in a single vacuum chamber and operated using a common set of control electronics, including a single rf amplifier and transformer coil. This multiplexed RIT mass spectrometer employs an array of four millimeter-sized ion traps (x(o) = 5.0 mm and y(o) = 4.0 mm, where x(o) and y(o) are the half-distances in the x and y dimensions, respectively). Mass spectra are acquired from four different samples simultaneously. The available mass/charge range is m/z 15-510 with excellent linearity of the mass calibration (R2 = 0.999 999). The peak width is less than 0.3 mass/charge units at m/z 146, corresponding to a resolution of approximately 500. Simultaneous MS/MS of ions due to four compounds (3-fluoroanisole, 4-fluoroanisole, 2-fluorobenzyl alcohol, 2,6-dimethylcyclohexanone) with the same nominal molecular radical cation but distinctive fragmentation patterns was demonstrated. Isolation and fragmentation efficiencies were approximately 25 and approximately 75%, respectively, measured in the typical case of the molecular radical cation of acetophenone. Preacquisition differential data were obtained by real-time subtraction of the ion signals from two channels of the multiplexed mass spectrometer. The differential experiment presented offers proof of principle of comparative mass spectra in high-throughput screening applications while reducing data storage requirements.
A method is reported for evaluating ion trap mass analyzers by selection of operating conditions under which both boundary and resonance ejection peaks occur in a single mass scan. The choice of frequency and amplitude of the auxiliary waveform applied for resonance ejection can be such as to produce a resonance ejection mass spectrum with unit resolution or, under selected conditions, signals attributable to both boundary and resonance ejection in a single mass scan. The contrasting mass resolution associated with these two ejection processes is evident in these data. The co-occurrence of the two ejection phenomena is ascribed to the effects of higher-order fields; it is more marked in some rectilinear ion traps (RITs) than in other nominally identical devices, leading to the possibility of using it to compare individual mass analyzers in multiplexed instruments. The method is used to compare multiple ion traps driven by the same RF signal in a fully-multiplexed mass spectrometer, composed of parallel ion source/mass analyzer/detector channels each housed in one quadrant of a specialized vacuum chamber. T he superposition of higher-order components (or multipoles) upon the main quadrupole potential of an ion trap is both unavoidable and, when properly engineered, advantageous to analytical performance. Truncated electrodes and electrode apertures produce nonlinear fields, including local field imperfections in the region of the electrodes, which affect the motion of ions, especially those with large excursions from the center of the ion trap as occurs just before ion ejection. The nature and magnitude of the higher-order contributions to the field of an ion trap is primarily a result of trap geometry, including the effects of mechanical dimensions and electrode alignment.One effect of nonlinear fields present in an ion trap of non-ideal geometry is the chemical mass shift, the premature or delayed appearance of signals for particular ions in a mass spectrum. Chemical mass shifts were apparent in early Paul traps built to the theoretical geometry r o 2 ϭ 2z o 2 until z o was stretched to compensate for the multipoles imposed by apertures in the endcap electrodes [1,2]. This phenomenon has been explained using simulation and experiment, and it is now understood that the local field imperfections affect the motion of ions nearing ejection [3,4].Octapolar or other contributions to the primarily quadrupolar potential of an ion trap are utilized when resonance ejection is performed at a nonlinear resonance point. The frequency used corresponds to that at which overtones from the higher-order multipoles are coincident with sidebands of the quadrupole potential. In this way, resolution can be enhanced relative to that achieved in boundary ejection [5].For ease of fabrication and miniaturization, the cylindrical ion trap (CIT) has been utilized as a geometrically simple substitute for the hyperbolic electrode Paul trap [6 -10]. To minimize the effects of higher-order field components, the dimensions of the CIT have been...
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