Mid-infrared chemical sensors based on quantum cascade (QC) devices offer improved sensitivity, portability and costs compared to FTIR-based spectrometers. In this work, we combine for the first time a broadband external-cavity QC laser (EC-QCL) with a spectrally tailored QC detector (QCD) for broadband detection of bovine milk proteins including β-lactoglobulin, α-lactalbumin and casein. We analyze concentrations between 0.25-15 g/L in a 12.5-µm transmission flow cell in the amide-I and -II band (~1730-1470 cm-1) and obtain: a RMS noise-level of 0.067 mAU, a limit-of-detection of ~0.09 g/L, excellent agreement with FTIR absorbance-spectra and similar performance as much more bulky high-end FTIR-spectrometers.
Photothermal Spectroscopy (PTS) is an indirect analytical technique in which the optical signal is directly proportional to the laser emission intensity. This direct dependence on the laser power means that - in contrast to more conventional transmission-absorption techniques - PTS fully benefits from the high power of novel tunable mid-infrared laser sources such as Quantum Cascade Lasers (QCLs). In particular, QCLs equipped with an external cavity (EC) allow broad tunability which can be exploited in the detection of liquids identified by broad absorption bands. To achieve high sensitivity in PTS it is also important to choose a sensitive mode of transducing photothermal signal. Among the PTS transduction techniques photothermal interferometry (i.e. the detection of the phase change resulting from sample heating) stands out due to its high sensitivity. In this work, we use an EC-QCL in a photothermal interferometry PTS setup for trace water detection. We employ a HeNe laser-based Mach-Zehnder Interferometer (MZI) with liquid flow-cells inserted in the two arms. An EC-QCL emitting in the range of 1570-1730 cm-1 is arranged co-linear to the analyte arm of the interferometer and used to target the bending mode (𝜈2 ~ 1645 cm-1) of water molecules in different matrices. Highest linearity and sensitivity are ensured by locking the MZI at its quadrature point via an active-feedback loop. Fluctuations and drifts are further minimized by means of temperature stabilization. When benchmarking the system against commercial FTIR spectrometers it is shown to be in excellent agreement with regards to band shapes, band positions and relative intensities and to compare favorably in terms of sensitivity. Achieved limits of detection (LODs) for water in chloroform and jet-fuel are in the low ppm range. Higher LODs orders of magnitude were obtained indeed for the case of water in ethanol. An analysis of the matrix influence on the PTS signal’s strength has been carried out. Results show how the choice of the matrix dramatically influences limits of detection and limits of quantification (LOQs).
Semiconductor-loaded plasmonic (SLSPP)-waveguides are a very efficient link for optoelectronic devices, facilitating miniaturized photonic integrated circuits. However, for long-wave infrared applications (8-12 µm), the material selection is challenging as most commonly used mid-IR materials absorb in this region. Therefore, we selected and investigated the properties of germanium in a hybrid semiconductor-metal-configuration to overcome these limitations. The experimental characterization of Si(substrate)-Au-Ge fabricated SLSPP-waveguides show very good agreement with FEM-simulations. Moreover, the realized devices offer low losses between 8.8 and 22 dB/mm (single device) and even within 8.8-15 dB/mm (multiple devices), respectively, for the entire investigated octave-spanning 5.6 – 11.2 µm range.
Mid-infrared dispersion spectroscopy is a novel alternative approach to classical absorption spectroscopy for qualitative and quantitative analysis of liquid-phase samples focused on broadband refractive index variation sensing originating from IR absorption. We present the redesigned and improved version of an external cavity-quantum cascade laser-based MachZehnder interferometer setup dedicated for refractive index sensing of liquids, which outperforms classic absorption spectroscopy. The refined version of the setup features greater compactness, a new dual-channel transmission cell and a hysteresis-free piezo-actuator for phase locked interferometric detection. Moreover, a new routine for fast and almost simultaneous acquisition of real and imaginary part of the complex refractive index (i.e., dispersion and absorption spectra) was introduced for mutual validation of the spectra. Dispersion spectra at sample temperatures ranging from 15 to 90°C can be recorded as the setup shows a stable noise-floor over that temperature range. Introduction of a hysteresis-free piezoactuator to the system enabled fast spectral acquisition at constant sensitivity with speed rates of 100 cm-1 /s, long-term stability and allowed to improve the reproducibility, robustness, and limits of detection of the method. We compare the performance of the refined setup with the previously demonstrated version by comparing the figures of merit for univariate glucose detection. In this context, the dispersion and absorption spectra of glucose were acquired and assessed. The achieved limit of detection for dispersion sensing was 5 times lower when compared to previous version and ~2 times lower than for classic absorption sensing at 5 times shorter spectra acquisition times. In summary, the improvements in the instrumentation for dispersion spectroscopy have improved the sensitivity, reliability, and quality of the method. The achieved results set a basis for further extension of the range of application presented for this technique.
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