A laser ablation mass spectrometer (LAMS) based on a time-of-flight (TOF) analyzer with adjustable drift length is proposed as a standoff elemental composition sensor for space missions to airless bodies. It is found that the use of a retarding potential analyzer in combination with a two-stage reflectron enables LAMS to be operated at variable drift length. For field-free drift lengths between 33 em to 100 em, at least unit mass resolution can be maintained solely by adjustment of internal voltages, and without resorting to drastic reductions in sensitivity. Therefore, LAMS should be able to be mounted on a robotic arm and analyze samples at standoff distances of up to several tens of em, permitting high operational flexibility and wide area coverage of heterogeneous regolith on airless bodies. 1 https://ntrs.nasa.gov/search.jsp?R=20120017379 2018-05-10T03:29:25+00:00Z Miniature mass spectrometers have been designed for use on space missions for decades [1][2][3][4][5]. Time-of-flight mass spectrometry (TOF-MS) has attracted increasing attention [6-10] due to its relative simplicity, wide mass range, high resolution, and compatibility with a variety of sampling and ionization methods. These advantages are especially beneficial on landed missions to airless bodies such as asteroids, comets, and most planetary satellites including the Moon. On such missions, a fixed lander or a rover may be deployed to explore a local region of the surface, where chemical analysis of a variety of regolith materials is expected to be a top priority. A laser ablation TOF-MS can be used for this analysis, without requiring collection and manipulation of samples [8,9, 11 J. In the laser ablation mass spectrometer (LAMS) instrument described previously [8,9], a high-intensity pulsed laser is directed onto a sample of interest, forming ions that travel across the vacuum gap between the instrument and the analyzer inlet, and are subsequently focused in a reflectron. Normally, the gap distance L ext (several cm in LAMS) has been treated as fixed, which would require precise instrument positioning such as with a robotic arm. However, it has been long known that the technique is compatible with variable L ext . The Figure 1, the field-free drift length L is the sum of ion path lengths outside (L ext ) and inside (Lint) the spectrometer. We show via theoretical simulation that high mass resolution (R > 250, sufficient to resolve unit mass isotopes) elemental analysis can he achieved for L ranging from 33 cm to at least 100 cm.In the LAMS design as described previously [8], the laser ablated ions travel from the sample surface into the mass analyzer and are redirected in a two-stage reflectron onto a dual microchannel plate (MCP) detector, arriving at a sequence of times proportional to the square root of their mass-to-charge ratios, i.e., (m/z) tn Neglecting the initial temporal and spatial spreads, the TOF of a particle with mass m and initial kinetic energy zV is given by the following equation (1):(1) Using the same method, we...