SCRIBES
Sensitive, Cooled, Resolved Ion BEam Spectroscopy
Introduction
Molecular ions play vital roles in many diverse areas of chemistry and astronomy, and are particularly relevant to chemistry in the interstellar medium (ISM). Because the ISM has a low number density (~100 cm-3) and temperature (~30 K), reactions with small barriers (such as ion/molecule reactions) dominate the chemistry. Because spectroscopy is the only tool available for probing astronomical environments, it is important to obtain laboratory spectra of these ions so that they may be detected in space. Vibrational spectroscopy is a particularly effective tool for this, as a molecule's vibrational spectrum contains a unique fingerprint based on its structure. Furthermore, a vibrational spectrum can be used to extract the rotational spectrum of a molecule, which is difficult to obtain because of difficulties in producing sufficient numbers of molecules and the microwave search problem. With SCRIBES, we are developing cutting-edge laboratory techniques for laser spectroscopic study of molecular ions in the gas phase under astrophysically relevant conditions. SCRIBES consists of an ion source, a fast ion beam, highly sensitive cavity enhanced spectroscopies, and a mass spectrometer.
The SCRIBES experiment as of 7 October 2009. The source chamber is in the background; the benders and drift region are to the right. The long tube in the foreground is the time-of-flight mass spectrometer.
Ion Source
Direct current discharges have commonly been used to produce ions for spectroscopy. However, the ions are produced with high rotational and vibrational temperatures. This is problematic not only because of increased spectral congestion, but also because, for weak transitions, the band strength is spread out over a large number of transitions instead of only a few, making the ion more difficult to observe. To overcome this, we are implementing a supersonic expansion discharge source, which will produce translationally and rotationally cold ions (<20 K). This not only solves the previously-mentioned issues, but also allows us to observe the spectrum as it would appear in the interstellar medium.
Ion Beam
A typical plasma is only about 1x10-6 ionized, so the vast majority of the plasma consists of un-ionized molecules. These can complicate the spectrum by absorbing in the same region that ions of interest absorb. In order to reduce this spectral confusion, we are using a fast ion beam to spatially separate the ions from the neutrals using electrostatic ion optics. An additional benefit of a fast ion beam is a reduction in the absorption linewidth through an effect called kinematic compression.
Spectrometer
When the ions are spatially separated from the neutrals, they are turned and sent into a drift region, where they are available to be probed by laser spectroscopy. We have attempted several types of cavity enhanced spectroscopies, including continuous-wave Cavity RingDown Spectroscopy (cw-CRDS), Cavity Enhanced Absorption Spectroscopy (CEAS), and Noise Immune Cavity Enhanced Optical Heterodyne Molecular Spectroscopy (NICE-OHMS). Currently we use a tunable cw Ti-Sapphire as our laser source in the near-infrared. But we also have a home-built difference frequency generation (DFG) laser which can be used to produce mid-infrared light. A DFG laser is made by combining the continuous-wave outputs of a Nd:YAG laser (1064 nm) and the Ti:Sapphire laser (700-900 nm) in a periodically-poled LiNbO3 nonlinear crystal. With this laser spectrometer, we are able to achieve high sensitivity (minimum detectable absorbance between ~1x10-7 and ~1x10-10) and high spectral resolution (3 x 10-5 cm-1).
A cold cathode discharge source used to produce hot ions. It is currently being used as a test source for aligning the ion beam.
Mass Spectrometer
When using a plasma source to produce ions for spectroscopy, it can be difficult to determine whether the observed spectrum comes from the ion of interest, or some other ionic species. We use a beam modulated time-of-flight mass spectrometer (BM-TOF-MS) to identify the species that are produced in our continuous ion source in SCRIBES. The BM-TOF-MS device uses quickly-pulsed deflecting plates to sweep the ion beam over a slit aperture placed near a dual micro-channel plate detector, thereby creating a small packet of ions. The ions in this packet are separated by mass during flight through a 1.5 meter drift region, resulting in a mass resolution on the order of 1 amu. By recording the mass spectrum of the ion beam, we can confirm the presence of our ion of interest in the beam, and also use the spectrum as a feedback mechanism for optimizing the production of that ion in the plasma. Additionally, the mass spectrometer can give information about the beam energy of the ion beam, as well as the energy spread. By measuring the spread of arrival times of single ions, one can determine the energy spread of the ion beam, which corresponds to a linewidth in the spectroscopy. Knowing the beam energy allows us to determine where lines will appear as a consequence of the Doppler-shift of the ions. Also, we have used the mass spectrometer to diagnose the performance of the uncooled cold cathode that produces the ions of interest. By using hydrogen as our discharge gas, we have found that the source contains different degrees of ion collisions depending on the orientation of the electrodes. This information is useful for determining the optimum source setup to produce ions of various electronic and vibrational energies. Having this mass spectrometer has proven invaluable in deducing the barriers to spectroscopy.
Highly Accurate and Precise Spectra
Traditionally, the accuracy of work in the mid-infrared is limited by the frequency standards that are used. Wavemeters typically have an absolute accuracy of 60-200 MHz, thereby limiting the ultimate accuracy of the measurement. This level of precision does not allow the pure rotational transitions to be inferred from the mid-infrared measurements with sufficient precision to enable radioastronomical searches. This problem can be reduced by using state of the art frequency measurements on the mid-infrared transitions. We do this using a MenloSystems Optical Frequency Comb. By using a GPS disciplined high stability crystal oscillator as our frequency reference, and a 70 MHz accuracy wavemeter, in conjunction with the frequency comb, we are able to determine line centers on transitions to better than 1 MHz. By improving the accuracy from 60 to 1 MHz, we ultimately increase the accuracy of measurements, further allowing for microwave observations to be enabled by mid-infrared spectroscopy.

NICE-OHVMS signal of N2+ in the fast ion beam. The light blue trace is the raw signal from the experiment, while the dark trace is the same signal smoothed.
Current Work
We have recently acquired our first signal of N2+ produced by an uncooled cold cathode source in the ion beam using velocity modulated NICE-OHMS. Presently, we are optimizing the sensitivity and lineshape of the signal. We can successfully acquire spectra of the N2+ ion beam using two modes of modulation: velocity modulation and concentration modulation. We also shortly aim to acquire N2+ ion beam spectra precisely calibrated to the optical frequency comb. With these precisely calibrated spectra, the line centers of the probed transitions should be measured to a high degree of accuracy.
After the spectrometer is optimized for N2+ spectroscopy in the near-infrared, we plan to build the mid-infrared DFG system and use the ion beam spectrometer to acquire vibrational spectra of various molecular ions of astrochemical interest. We will begin by studying a simple test ion, HN2+. Later, we aim to record ultra-high resolution spectra of astronomically interesting molecular ions, such as HCO+, HOC+, and others. Further in the future, we will integrate the supersonic expansion discharge ion source to the instrument to study the supersonically cooled spectra of CH5+, C3H3+, and other nonlinear molecuar ions. At this point, the building of SCRIBES should be complete, and will hopefully function as a powerful tool for high resolution rotationally cooled spectroscopy of molecular ions.

