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种高效、灵敏的激光解吸取样离子迁移谱(IMS)系统被应用于使用不同表面材料的快速爆炸物检测。这种便携式智能检测系统探测器由电池供电,具有移动性,适合在野外或战区使用 标签: 离子迁移谱、爆炸物、六氯乙烷、掺杂剂、IMS、PAIMS |
Laser Desorption of Explosives from the Surface of Different Real-World Materials Studied Using C2Cl6-Dopant-Assisted Ion Mobility Spectrometry
Emanuel Maťaš 1,Matej Petrík 2,Martin Sabo 2,3 Štefan Matejčík 1,*
1 Faculty of Mathematics, Physics and Informatics, Comenius University in Bratislava, 842 48 Bratislava, Slovakia
2 Faculty of Informatics and Information Technologies, Slovak University of Technology in Bratislava, 842 16 Bratislava, Slovakia
3 MaSa Tech s.r.o., Sadová 3018/10, 916 01 Stará Turá, Slovakia
*
Author to whom correspondence should be addressed.
Molecules 2024, 29(18), 4482; https://doi.org/10.3390/molecules29184482 (registering DOI)
Submission received: 7 August 2024 / Revised: 7 September 2024 / Accepted: 9 September 2024 / Published: 21 September 2024
3. Materials and Methods
3.1. Experimental Setup
The ion mobility spectrometry (IMS) system used in this study to detect explosives was developed by MaSa Tech Ltd., Company (Stará Turá, Slovakia). The IMS device was boxed with all electronics, power supplies, filters, and dopant gas (Figure 4a). The device was powered by a battery that allowed continuous operation for up to 8 h. This makes the IMS a highly portable analytical device. The IMS instrument was constructed using multiple stainless-steel ring electrodes isolated by Teflon rings, resulting in a total length of the drift tube of 11.16 cm, as shown in Figure 4b. The corona discharge (CD) ionization source was operated in negative polarity, following a point-to-plane geometry, with the gas outlet positioned behind the discharge, allowing the CD to operate in a reverse-flow regime. For IMS equipment, a Bradbury–Nielsen-type shutter grid (SG) with an opening time of 150 µs and a period of 14,500 µs was employed. A potential difference of 3.6 kV was applied across the CD, and the electric field intensity inside the drift tube was set to 509.8 V.cm−1. As a drift gas was used, purified atmospheric air was obtained through a zeolite filter (Agilent Technologies, Inc., Santa Clara, CA, USA) with a typical flow rate of 600 mL/min. The operational pressure was maintained at 600 mbar, and the IMS drift tube temperature was set to 60 °C. The desorbed sample was sucked through a 50 cm long PEEK capillary with an inner diameter of 0.8 mm. The sample gas flow comprised 500 mL/min of atmospheric air without additional purification but with an admixture of C2Cl6 dopant with a concentration of 750 ppb. The capillary input was positioned perpendicular to the laser beam, several millimeters from the sample surface. A standard diode laser operating at a wavelength of 532 nm (green light) with a power of 1000 mW was employed in the setup. The spot of the focused laser beam was 1.4 mm2. The irradiation time was exactly one second for all measurements.
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