Ryan T. Hilger

Absorption mode Fourier transform electrostatic linear ion trap mass spectrometry.

In Fourier transform mass spectrometry, it is well-known that plotting the spectrum in absorption mode rather than magnitude mode has several advantages. However, magnitude spectra remain commonplace due to difficulties associated with determining the phase of each frequency at the onset of data acquisition, which is required for generating absorption spectra. The phasing problem for electrostatic traps is much simpler than for Fourier transform ion cyclotron resonance (FTICR) instruments, which greatly simplifies the generation of absorption spectra. Here, we present a simple method for generating absorption spectra from a Fourier transform electrostatic linear ion trap mass spectrometer. The method involves time shifting the data prior to Fourier transformation in order to synchronize the onset of data acquisition with the moment of ion acceleration into the electrostatic trap. Under these conditions, the initial phase of each frequency at the onset of data acquisition is zero. We demonstrate that absorption mode provides a 1.7-fold increase in resolution (full width at half maximum, fwhm) as well as reduced peak tailing. We also discuss methodology that may be applied to unsynchronized data in order to determine the time shift required to generate an absorption spectrum.

Nondestructive Tandem Mass Spectrometry Using a Linear Quadrupole Ion Trap Coupled to a Linear Electrostatic Ion Trap

A novel hybrid tandem mass spectrometer is presented that combines a linear quadrupole ion trap (QLIT) with a linear electrostatic ion trap (ELIT), which is composed of opposing ion mirrors. The QLIT is used both as an accumulation device for the pulsed injection of ions into the ELIT and as a collision cell for ions released from the ELIT and back into the QLIT. Ions are subjected to mass analysis in the ELIT via Fourier transformation of the time-domain signal obtained from an image current measurement using a pick-up electrode in the field-free region of the ELIT. The nondestructive nature of ion detection and the relatively straightforward axial entrance and exit of ions into and from the ELIT allow for the execution of nondestructive tandem mass spectrometry experiments whereby both the initial mass spectrum and the product ion spectrum are obtained on the same initial ion population. The timed pulsing of a deflection electrode, in conjunction with the release of ions from the ELIT, allows for the selection of precursor ions for recapture by the QLIT. The transfer of ions back and forth between the QLIT and ELIT is illustrated with Cs ions, the selection of precursor ions is demonstrated with isotopes of tetraoctylammonium cations, and complete nondestructive tandem mass spectrometry experiments are demonstrated with a mixture of angiotensin II and bradykinin cations. With the current apparatus, the efficiency for the process of recapturing ions and then reinjecting them into the ELIT is 35%-40%. The instrument is capable of isolating an ion from a neighbor with a mass as close as 1 part in 500, with negligible loss of the desired species.

Electroosmotically driven solution mixing in borosilicate theta glass nESI emitters

The use of borosilicate theta glass capillaries as nanoelectrospray ionization emitters has recently been demonstrated as a method for mixing two solutions as they are sprayed into the mass spectrometer for analysis. All previous experiments resulted in a solution mixing timescale limited to the time the analytes spend in the Taylor cone and subsequent droplets (i.e. sub-millisecond timescale). In an effort to extend the solution mixing timescale to the milliseconds regime, we demonstrate that solution can be moved from one channel of the theta tip to the opposite channel via electroosmosis by applying a potential difference between the two wire electrodes inserted into each channel of the theta tip. First, we establish that electroosmosis is responsible for solution movement using fluorescence microscopy to track fluorescent tracer dyes. We then demonstrate the utility of this technique in varying the extent of denaturation of holomyoglobin to apomyoglobin on the millisecond timescale just prior to analysis by mass spectrometry. Finally, we induce additional turbulence for better mixing by applying a square wave potential to one of the wire electrodes while holding the opposite wire at a constant voltage between the low and high potentials of the square wave. This experiment was found to provide nearly complete mixing after a single cycle of the square wave. The use of electroosmosis significantly expands the flexibility of theta tips for altering solutions prior to nESI without the need for off-line sample manipulation. Copyright

Tandem Mass Spectrometry in an Electrostatic Linear Ion Trap Modified for Surface-Induced Dissociation

A variety of ion traps are used in mass spectrometry. A key feature shared by most of them is the ability to perform tandem mass spectrometry (MS/MS). The Orbitrap is perhaps the most notable ion trap in which MS/MS has yet to be performed. An electrostatic linear ion trap (ELIT) is analogous to an orbitrap in that ions are trapped using solely electrostatic fields. However, the relatively simple ion motion within an ELIT facilitates analysis of fragment ions produced within the device. In this report, we describe an ELIT to which we have added a target for surface induced dissociation (SID). When combined with our previously described method for isolating a precursor ion trapped in an ELIT,1 this apparatus enables MS/MS to be performed. Measurement of product ion m/z is facilitated by the fact that the ELIT is isochronous over the energy range of 1850-2000 eV so that changes to ion energy during SID do not cause major m/z shifts. We demonstrate MS/MS by isolating and dissociating each compound in a four component mixture of tetraalkylphosphonium cations. We also discuss the optimization of collision energy and the length of time that the SID target is available for collision, two parameters that are important in the performance of these experiments.

Precursor and Neutral Loss Scans in an RF Scanning Linear Quadrupole Ion Trap

AbstractMethodology for performing precursor and neutral loss scans in an RF scanning linear quadrupole ion trap is described and compared to the unconventional ac frequency scan technique. In the RF scanning variant, precursor ions are mass selectively excited by a fixed frequency resonance excitation signal at low Mathieu q while the RF amplitude is ramped linearly to pass ions through the point of excitation such that the excited ion’s m/z varies linearly with time. Ironically, a nonlinear ac frequency scan is still required for ejection of the product ions since their frequencies vary nonlinearly with the linearly varying RF amplitude. In the case of the precursor scan, the ejection frequency must be scanned so that it is fixed on a product ion m/z throughout the RF scan, whereas in the neutral loss scan, it must be scanned to maintain a constant mass offset from the excited precursor ions. Both simultaneous and sequential permutation scans are possible; only the former are demonstrated here. The scans described are performed on a variety of samples using different ionization sources: protonated amphetamine ions generated by nanoelectrospray ionization (nESI), explosives ionized by low-temperature plasma (LTP), and chemical warfare agent simulants sampled from a surface and analyzed with swab touch spray (TS). We lastly conclude that the ac frequency scan variant of these MS/MS scans is preferred due to electronic simplicity. In an accompanying manuscript, we thus describe the implementation of orthogonal double resonance precursor and neutral loss scans on the Mini 12 using constant RF voltage. Graphical Abstractᅟ