D Jet ion guide
When ions enter the mass spectrometer through the orifice, from atmospheric pressure into the vacuum, they experience a large free-jet expansion. It is very important that there is an element behind the orifice that can quickly and efficiently capture and focus these ions into a narrow beam. These elements have evolved over the years, from skimmer cones to quadrupoles to the QJet ion guide—and now the D Jet ion guide.
The D Jet ion guide has a dual stage design that transports ions between the orifice and Q0. In the first vacuum stage, a dodecapole RF ion guide has been developed to capture and focus ions that are sampled though the orifice. The QJet ion guides in other SCIEX systems are single stage quadrupole ion guides. Quadrupole ion guides focus ions along the central axis of the ion guide. They are less effective, however, for operation at higher gas pressures. Conversely, higher order multipoles such as octapoles and dodecapoles confine ions more towards the periphery, and have deeper but flatter potential wells for an equivalent voltage, making them ideal for the SCIEX 7500 system.
High pressure ion guides like the D Jet ion guide require a large number of electrodes to generate a high-order multipole field. They also need to be designed to constrain the gas flow and pressure in the second stage ion guide to minimize shock waves that would result in poor transmission efficiency. To constrain gas flow within the D Jet ion guide, the electrode surfaces gradually narrow and tilt inward to provide a smaller radius at the exit. In addition, each of the plurality of electrodes gradually becomes thicker toward the narrower exit end of the ion guide.
Experimental results and simulations suggest that the transmission efficiency of the D Jet ion guide is superior to previous designs. The conclusion from computational fluid dynamics (CFD) simulations (Figure 2) is that gas flow is critical to the efficiency of high-pressure ion guides. Although electrical containment is necessary, optimized hardware design to eliminate beaming and other deleterious gas flow effects is critical. The D Jet ion guide has been optimized for use at high pressure and provides broad optima for the RF potential. As a result of this optimization, simulations have demonstrated greater than 90% efficiency for ion transmission through both stages of the D Jet ion guide.8
OptiFlow Pro ion source with E Lens probe
The fourth generation in the Turbo V ion source family, the OptiFlow Pro ion source provides the highest flexibility and functionality, due to the modular architecture, while maintaining the robustness and reproducibility of previous generations. The source is compatible with a broad flow range, from microflow (1 µL/min) to analytical flow (up to 3 mL/min), with interchangeable probes and electrodes. The OptiFlow Pro ion source is optimized for performance and robustness; no positional tuning is required at any flow rate. Interchangeable ESI and APCI towers allow users to easily switch between ionization modes for broad compound coverage.
E Lens probe places an electrode near the orifice to drive ions from the spray plume towards the orifice. This lens creates a stronger field that the ions must traverse, which imparts more energy into the droplet and causes more efficient break-up and release of more ions, resulting in enhanced ion collection (Figure 3). This improved desolvation leads to increased sensitivity with performance gains up to 2-fold, with the largest gains observed for peptides when combined with microflow rates.7
Robustness across many injections
The ability to run a specific assay on many complex samples across multiple days is also key to success in many applications. Key to robustness on SCIEX mass spectrometers is the combination of the highly efficient OptiFlow Pro ion source design and the optimized geometry of the Curtain Gas interface. Here, a study was performed in a very complex matrix (black tea) to test the robustness of the system with the D Jet ion guide on the SCIEX 7500 system (Figure 4). Minimal degradation in peak area or decrease in signal to noise was observed across 2700 injections, with peak area variance across the dataset of 4.05%. These results highlight that the instrument sensitivity is increased with no loss in robustness, providing rugged performance for complex biological matrices.
Linear dynamic range
Linear dynamic range (LDR) is important in many applications where the analyte concentration varies widely. On the SCIEX 7500 system, up to 6 orders of magnitude across the LDR is achievable (Figure 5), which improves quantitative coverage and increases lab throughput. This detection system equipped with a multi-channel electron multiplier and dead time correction algorithm achieves a very high pulse counting rate. As a result, intense peaks of up to 1 x 108 cps can be measured with no observed detector saturation.
In addition, because of the presence of the high energy dynode as part of the detector, the system can switch between polarities extremely fast (5 msec), enabling detection of a larger number of diverse analytes in a single injection.
Conclusions
The SCIEX 7500 system is the next high end quantitative platform from SCIEX. With the same ruggedness and robustness of previous generations, the SCIEX 7500 system provides higher sensitivity to meet the needs of the most challenging assays.
- D Jet ion guide and integrated E Lens probe combine to deliver significant sensitivity gains over the previous generation of instruments: average MRM peak area gains of 7x and signal to noise gains of 2.5 to 3x.
- The OptiFlow Pro ion source, built on the reliability and efficiency of the legendary Turbo V ion source, now provides high flexibility to meet diverse application needs with a single source solution. The modular design allows fast switching between high and low flow regimes and adapts to workflow requirements (ESI vs. APCI ionization modes).
- Up to 6 orders of linear dynamic range and fast polarity switching (5 msec) are available.
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