Lukas Escher’s research while affiliated with University of Regensburg and other places

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Publications (6)


Photodissociation-Driven Photoacoustic Spectroscopy with UV-LEDs for Ozone Detection
  • Article

March 2025

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11 Reads

Photoacoustics

Lukas Escher

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Simon Jobst

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[...]

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Frank-Michael Matysik

This study presents the development and evaluation of a UV-LED based photoacoustic (PA) measurement system for ozone (O3) detection to demonstrate its potential for low-cost and accurate sensing while for the first time addressing the importance of photodissociation for PA signal generation for O3 in the UV range. With a detection limit of 7.9 ppbV, the system exhibits a significant advancement over state-of-the-art UV-PA O3 detection and is on par with laser-based setups. Following a novel discussion of the PA signal arising from photodissociation and its products, cross-sensitivity effects due to environmental factors such as temperature and gas composition were systematically analyzed. A digital twin driven compensation for these influences was implemented and evaluated. Despite the challenges associated with modeling the effects of H2O and CO2, the PA system shows considerable potential, though further studies in real world applications must be conducted.


Photoacoustic Trace-Analysis of Breath Isoprene and Acetone via Interband- and Quantum Cascade Lasers
  • Article
  • Full-text available

November 2024

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62 Reads

Sensors and Actuators B Chemical

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Fig. 1. Simplified Jablonski diagram of a two-level system to predict the relaxation cascade of photoacoustic signal generation for methane monitoring in air. The grey shaded area highlights the dyad of CH 4 vibrations v b [28].
Fig. 2 shows amplitude-modulated photoacoustic spectra of 15 ppmV methane diluted in pure nitrogen (yellow) as well as with successive substitutions of nitrogen by oxygen. Refer to the legend of the figure for the assignment of the spectra and their respective O₂ concentrations. The scaled sensor voltage |U LIA | accounts for changes in P 0 during laser tuning and has been scaled to the maximum optical power at 1209.2 cm 1 . This scaling point is extrapolated as a dotted black horizontal reference line across the measured spectrum. Since this scaling occurs outside the methane absorption feature, it corresponds to the photoacoustic background signal (BS), which arises from the interaction of QCL radiation with the windows of the PA cell during amplitude modulation. The purple line represents the absorption cross-section of methane as provided by HITRAN database. It can be observed that the PA signal decreases with the addition of O 2 , surprisingly this trend continues to a measured magnitude of less than the background signal when exceeding O 2 concentrations of 6 %V. The violet and green spectra at 10 %V and 20 %V O₂ appear to be mirror-
Fig. 4. Measured PA signals from Fig. 3 after offset-correction (blue crosses) and DT-simulated signals (red dots) are presented in a complex vector diagram (a) and their absolute values plotted as a function of O₂ concentration (b).
Fig. 5. Representation of the contributions of individual collision reactions to the photoacoustic signal amplitude for selected N₂:O₂ matrix compositions as a bar chart. The red dashed horizontal line indicates the energy of a light quantum in eV. The overlaid white diagonally hatched area illustrates the absolute heat dissipation q 100 .
Kinetic Cooling in Mid-Infrared Methane Photoacoustic Spectroscopy: A Quantitative Analysis via Digital Twin Verification

September 2024

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34 Reads

Photoacoustics

This study presents a detailed quantitative analysis of kinetic cooling in methane photoacoustic spectroscopy, leveraging the capabilities of a digital twin model. Using a quantum cascade laser tuned to 1210.01 cm⁻1, we investigated the effects of varying nitrogen-oxygen matrix compositions on the photoacoustic signals of 15 ppmV methane. Notably, the photoacoustic signal amplitude decreased with increasing oxygen concentration, even falling below the background signal at oxygen levels higher than approximately 6 %V. This phenomenon was attributed to kinetic cooling, where thermal energy is extracted from the surrounding gas molecules rather than added, as validated by complex vector analysis using a previously published digital twin model. The model accurately reproduced complex signal patterns through simulations, providing insights into the underlying molecular mechanisms by quantifying individual collision contributions. These findings underscore the importance of digital twins in understanding the fundamentals of photoacoustic signal generation at the molecular level.