Continuous glucose monitoring by means of mid-infrared transmission laser spectroscopy in vitro

The continuous surveillance of glucose concentration reduces short-term risks and long-term complications for people with diabetes mellitus, a disorder of glucose metabolism. As a first step towards the continuous monitoring of glucose, reagent-free transmission spectroscopy in the mid-infrared region has been carried out in vitro using a quantum cascade laser and an optical silver halide fiber. A 30 μm gap in the fiber allowed for transmission spectroscopy of aqueous glucose solutions at a wavelength of 9.69 μm, which is specific to a molecular vibration of glucose. A noise-equivalent concentration as low as 4 mg/dL was achieved at an average power of 1.8 mW and an integration time of 50 s. This is among the most precise of glucose measurements using mid-infrared spectroscopy. Even with the very low average laser power of 0.07 mW the sensitivity of previous results (using a fiber optical evanescent field analysis) has been improved upon by almost one order of magnitude. Finally, the impact of potentially interfering substances such as other carbohydrates was analyzed.     

Electrical transport and magnetic ordering in R 2Ti3Ge4 (R=Dy, Ho and Er) compounds

New R ₂Ti₃Ge₄ (R=Dy, Ho and Er) intermetallic compounds have been synthesized and characterized by X-ray diffraction and low temperature ac magnetic susceptibility, electrical resistivity and thermoelectric power measurements were carried out. The compounds crystallize in the parent, Sm₅Ge₄-type orthorhombic structure (space group Pnma) and lanthanide contraction is observed as one moves along the rare-earth series. The changeover from paramagnetic to antiferromagnetic phase happens at low temperatures and the ordering temperature scales with the de Gennes factor. The electrical resistivity is metallic with a negative curvature above 100 K. Thermopower displays a weak maximum at temperatures less than 50 K signifying the possible phonon and magnon drag effects.     

Elastic properties of the Ta–V system: bcc Ta0.33V0.67 and C15 TaV2

Resonant ultrasound spectroscopy was used to measure the elastic constants of bcc Ta_0.33V_0.67 over the temperature range 3.5–300?K; the results were compared to earlier measurements on C15 TaV₂. The temperature dependence of the polycrystalline shear modulus is completely different in the two phases; that of the bcc phase decreases with temperature whereas that of the C15 phases increases in an anomalous fashion. This difference is consistent with a model involving doubly-degenerate levels at the X point of the Brillouin zone in the C15 phase with the Fermi level lying near the doubly degenerate level. This model accounted for the unusual behaviour of the C15 phase. Debye temperatures were determined from the ultrasonic measurements: 295?K for the C15 phase and 315?K for the bcc phase.     

Electric quadrupole interaction of Cd in (Ce1−xLax)Ru2 and (Ce1−yCay)Ru2 synthesized at high pressure

Quasibinary Laves systems (Ce_1−xLa_x)Ru₂ and (Ce_1−yCa_y)Ru₂ doped with ¹¹¹In were synthesized at a pressure of 8 GPa, and variations of the electric quadrupole interaction of ¹¹¹Cd at the Ru sites have been studied by the method of time-differential perturbed angular correlation in a wide range of Ce-La and Ce-Ca relative concentrations. In the first case two sites with quadrupole frequencies ν_Q≅220 and 150 MHz persist at x≤0.2, while at x≥0.3 only the higher frequency component remains in the spectra, which are similar to that of pure LaRu₂. In the series (Ce_1−yCa_y)Ru₂, at y≥0.03 the lower frequency component was washed out except in samples with y=0.1 and 0.2, where it was restored.     

Hyperfine fields and magnetic moments in intermetallic ScFe2 with cubic and hexagonal structures

The Sc, Fe and Al NMR spectra have been measured. The spectra and hyperfine fields are dependent on the crystal structures. The magnetic moments of Fe sites were estimated. The magnetic moments of Sc sites μ(Sc) in ScFe₂ (MgCu₂) were evaluated from the magnetic moment per formula μ_∫ as well. μ_∫ in ScFe₂ with hexagonal structures are sharply dependent on the technological conditions and the impurities in the samples.