TY - JOUR A1 - Leiterer, York A1 - Leitenberger, Wolfram A1 - Emmerling, Franziska A1 - Thünemann, Andreas F. A1 - Panne, Ulrich T1 - The use of an acoustic levitator to follow crystallization in small droplets by energydispersive X-ray diffraction Y1 - 2006 UR - http://journals.iucr.org/j/issues/2006/05/00/wf5016/wf5016.pdf U6 - https://doi.org/10.1107/S0021889806024915 SN - 0021-8898 ER - TY - JOUR A1 - Michalik-Onichimowska, Aleksandra A1 - Beitz, Toralf A1 - Panne, Ulrich A1 - Löhmannsröben, Hans-Gerd A1 - Riedel, Jens T1 - Microsecond mid-infrared laser pulses for atmospheric pressure laser ablation/ionization of liquid samples JF - Sensors and actuators : B, Chemical N2 - In many laser based ionization techniques with a subsequent drift time separation, the laser pulse generating the ions is considered as the start time to. Therefore, an accurate temporal definition of this event is crucial for the resolution of the experiments. In this contribution, the laser induced plume dynamics of liquids evaporating into atmospheric pressure are visualized for two distinctively different laser pulse widths, Delta t = 6 nanoseconds and Delta tau = 280 microseconds. For ns-pulses the expansion of the generated vapour against atmospheric pressure is found to lead to turbulences inside the gas phase. This results in spatial and temporal broadening of the nascent clouds. A more equilibrated expansion, without artificial smearing of the temporal resolution can, in contrast, be observed to follow mu s-pulse excitation. This leads to the counterintuitive finding that longer laser pulses results in an increased temporal vapour formation definition. To examine if this fume expansion also eventually results in a better definition of ion formation, the nascent vapour plumes were expanded into a linear drift tube ion mobility spectrometer (IMS). This time resolved detection of ion formation corroborates the temporal broadening caused by collisional impeding of the supersonic expansion at atmospheric pressure and the overall better defined ion formation by evaporation with long laser pulses. A direct comparison of the observed results strongly suggests the coexistence of two individual ion formation mechanisms that can be specifically addressed by the use of appropriate laser sources. KW - Laser ablation KW - Ion mobility spectrometry KW - Pulse duration KW - Plume KW - Ionization Y1 - 2016 U6 - https://doi.org/10.1016/j.snb.2016.06.155 SN - 0925-4005 VL - 238 SP - 298 EP - 305 PB - Elsevier CY - Lausanne ER - TY - JOUR A1 - Michalik-Onichimowska, Aleksandra A1 - Beitz, Toralf A1 - Panne, Ulrich A1 - Löhmannsröben, Hans-Gerd A1 - Riedel, Jens T1 - Laser ionization ion mobility spectrometric interrogation of acoustically levitated droplets JF - Analytical and bioanalytical chemistry : a merger of Fresenius' journal of analytical chemistry, Analusis and Quimica analitica N2 - Acoustically levitated droplets have been suggested as compartmentalized, yet wall-less microreactors for high-throughput reaction optimization purposes. The absence of walls is envisioned to simplify up-scaling of the optimized reaction conditions found in the microliter volumes. A consequent pursuance of high-throughput chemistry calls for a fast, robust and sensitive analysis suited for online interrogation. For reaction optimization, targeted analysis with relatively low sensitivity suffices, while a fast, robust and automated sampling is paramount. To follow this approach, in this contribution, a direct coupling of levitated droplets to a homebuilt ion mobility spectrometer (IMS) is presented. The sampling, transfer to the gas phase, as well as the ionization are all performed by a single exposure of the sampling volume to the resonant output of a mid-IR laser. Once formed, the nascent spatially and temporally evolving analyte ion cloud needs to be guided out of the acoustically confined trap into the inlet of the ion mobility spectrometer. Since the IMS is operated at ambient pressure, no fluid dynamic along a pressure gradient can be employed. Instead, the transfer is achieved by the electrostatic potential gradient inside a dual ring electrode ion optics, guiding the analyte ion cloud into the first stage of the IMS linear drift tube accelerator. The design of the appropriate atmospheric pressure ion optics is based on the original vacuum ion optics design of Wiley and McLaren. The obtained experimental results nicely coincide with ion trajectory calculations based on a collisional model. KW - Ambient pressure laser ionization KW - Ionmobility spectrometry KW - Acoustic levitation KW - Ion optics Y1 - 2019 U6 - https://doi.org/10.1007/s00216-019-02167-5 SN - 1618-2642 SN - 1618-2650 VL - 411 IS - 30 SP - 8053 EP - 8061 PB - Springer CY - Heidelberg ER - TY - JOUR A1 - Michalik-Onichimowska, Aleksandra A1 - Kern, Simon A1 - Riedel, Jens A1 - Panne, Ulrich A1 - King, Rudibert A1 - Maiwald, Michael T1 - "Click" analytics for "click" chemistry - A simple method for calibration-free evaluation of online NMR spectra JF - Journal of magnetic resonance N2 - Driven mostly by the search for chemical syntheses under biocompatible conditions, so called "click" chemistry rapidly became a growing field of research. The resulting simple one-pot reactions are so far only scarcely accompanied by an adequate optimization via comparably straightforward and robust analysis techniques possessing short set-up times. Here, we report on a fast and reliable calibration-free online NMR monitoring approach for technical mixtures. It combines a versatile fluidic system, continuous-flow measurement of H-1 spectra with a time interval of 20 s per spectrum, and a robust, fully automated algorithm to interpret the obtained data. As a proof-of-concept, the thiol-ene coupling between N-boc cysteine methyl ester and ally] alcohol was conducted in a variety of non-deuterated solvents while its time-resolved behaviour was characterized with step tracer experiments. Overlapping signals in online spectra during thiol-ene coupling could be deconvoluted with a spectral model using indirect hard modeling and were subsequently converted to either molar ratios (using a calibration free approach) or absolute concentrations (using 1-point calibration). For various solvents the kinetic constant k for pseudo-first order reaction was estimated to be 3.9 h(-1) at 25 degrees C. The obtained results were compared with direct integration of non-overlapping signals and showed good agreement with the implemented mass balance. (C) 2017 Elsevier Inc. All rights reserved. KW - NMR spectroscopy KW - Reaction monitoring KW - Automated data evaluation KW - Thiol-ene click chemistry Y1 - 2017 U6 - https://doi.org/10.1016/j.jmr.2017.02.018 SN - 1090-7807 SN - 1096-0856 VL - 277 SP - 154 EP - 161 PB - Elsevier CY - San Diego ER -